# Tag Archives: quantum electrodynamics

# Wavefunctions as gravitational waves

This is the paper I always wanted to write. It is there now, and I think it is good – and *that*‘s an understatement. š It is probably best to download it as a pdf-file from the viXra.org site because this was a rather fast ‘copy and paste’ job from the Word version of the paper, so there may be issues with boldface notation (vector notation), italics and, most importantly, with formulas – which I, sadly, have to ‘snip’ into this WordPress blog, as they don’t have an easy copy function for mathematical formulas.

It’s great stuff. If you have been following my blog – and many of you have – you *will* want to digest *this*. š

**Abstract : **This paper explores the implications of associating the components of the wavefunction with a physical dimension: force per unit *mass* ā which is, of course, the dimension of acceleration (m/s^{2}) and gravitational fields. The classical electromagnetic field equations for energy densities, the Poynting vector and spin angular momentum are then re-derived by substituting the electromagnetic N/C unit of field strength (mass per unit *charge*) by the new N/kg = m/s^{2} dimension.

The results are elegant and insightful. For example, the energy densities are proportional to the square of the absolute value of the wavefunction and, hence, to the probabilities, which establishes a *physical *normalization condition. Also, SchrĆ¶dingerās wave equation may then, effectively, be interpreted as a diffusion equation for energy, and the wavefunction itself can be interpreted as a propagating gravitational wave. Finally, as an added bonus, concepts such as the Compton scattering radius for a particle, spin angular momentum, and the boson-fermion dichotomy, can also be explained more intuitively.

While the approach offers a physical interpretation of the wavefunction, the author argues that the *core *of the Copenhagen interpretations revolves around the complementarity principle, which remains unchallenged because the interpretation of amplitude waves as traveling fields does *not *explain the particle nature of matter.

# Introduction

This is *not *another introduction to quantum mechanics. We assume the reader is already familiar with the key principles and, importantly, with the basic math. We offer an *interpretation *of wave mechanics. As such, we do *not *challenge the complementarity principle: the *physical *interpretation of the wavefunction that is offered here explains the *wave* nature of matter only. It explains diffraction and interference of amplitudes but it does *not *explain why a particle will hit the detector *not as a wave but as a particle*. Hence, the Copenhagen interpretation of the wavefunction remains relevant: we just push its boundaries.

The basic ideas in this paper stem from a simple observation: the *geometric *similarity between the quantum-mechanical wavefunctions and electromagnetic waves is remarkably similar. The components of both waves are orthogonal to the direction of propagation and to each other. Only the relative phase differs : the electric and magnetic field vectors (**E** and **B**) have the same phase. In contrast, the phase of the real and imaginary part of the (elementary) wavefunction (Ļ = *aĀ·e*^{āiāĪø} = *a*ācosĪø – *a*āsinĪø) differ by 90 degrees (Ļ/2).[1] Pursuing the analogy, we explore the following question: if the oscillating electric and magnetic field vectors of an electromagnetic wave carry the energy that one associates with the wave, can we analyze the real and imaginary part of the wavefunction in a similar way?

We show the answer is positive and remarkably straightforward. If the physical dimension of the electromagnetic field is expressed in newton per coulomb (force per unit charge), then the physical dimension of the components of the wavefunction may be associated with force per unit mass (newton per kg).[2] Of course, force over some distance is energy. The question then becomes: what is the energy concept here? Kinetic? Potential? Both?

The similarity between the energy of a (one-dimensional) linear oscillator (E = mĀ·*a*^{2}Ā·Ļ^{2}/2) and Einsteinās relativistic energy equation E = mā*c*^{2} inspires us to interpret the energy as a *two*-dimensional oscillation of mass. To assist the reader, we construct a two-piston engine metaphor.[3] We then adapt the formula for the electromagnetic energy density to calculate the energy densities for the wave function. The results are elegant and intuitive: the energy densities are proportional to the square of the absolute value of the wavefunction and, hence, to the probabilities. SchrĆ¶dingerās wave equation may then, effectively, be interpreted as a diffusion equation for energy itself.

As an added bonus, concepts such as the Compton scattering radius for a particle and spin angular, as well as the boson-fermion dichotomy can be explained in a fully intuitive way.[4]

Of course, such interpretation is also an interpretation of the wavefunction itself, and the immediate reaction of the reader is predictable: the electric and magnetic field vectors are, somehow, to be looked at as *real* vectors. In contrast, the real and imaginary components of the wavefunction are not. However, this objection needs to be phrased more carefully. First, it may be noted that, in a classical analysis, the magnetic force is a pseudovector itself.[5] Second, a suitable choice of coordinates may make quantum-mechanical rotation matrices irrelevant.[6]

Therefore, the author is of the opinion that this little paper may provide some fresh perspective on the question, thereby further exploring Einsteinās basic sentiment in regard to quantum mechanics, which may be summarized as follows: there must be some *physical* explanation for the calculated probabilities.[7]

We will, therefore, start with Einsteinās relativistic energy equation (E = m*c*^{2}) and wonder what it could possibly tell us.** **

# I. Energy as a two-dimensional oscillation of mass

The structural similarity between the relativistic energy formula, the formula for the *total *energy of an oscillator, and the *kinetic* energy of a moving body, is striking:

- E = m
*c*^{2} - E = mĻ
^{2}/2 - E = m
*v*^{2}/2

In these formulas, Ļ, *v *and *c *all describe some velocity.[8] Of course, there is the 1/2 factor in the E = mĻ^{2}/2 formula[9], but that is exactly the point we are going to explore here: can we think of an oscillation in *two *dimensions, so it stores an amount of energy that is equal to E = 2Ā·mĀ·Ļ^{2}/2 = mĀ·Ļ^{2}?

That is easy enough. Think, for example, of a V-2 engine with the pistons at a 90-degree angle, as illustrated below. The 90Ā° angle makes it possible to perfectly balance the counterweight and the pistons, thereby ensuring smooth travel at all times. With permanently closed valves, the air inside the cylinder compresses and decompresses as the pistons move up and down and provides, therefore, a restoring force. As such, it will store potential energy, just like a spring, and the motion of the pistons will also reflect that of a mass on a spring. Hence, we can describe it by a sinusoidal function, with the zero point at the center of each cylinder. We can, therefore, think of the moving pistons as harmonic oscillators, just like mechanical springs.

**Figure 1**: Oscillations in two dimensions

If we assume there is no friction, we have a *perpetuum mobile *here. The compressed air and the rotating counterweight (which, combined with the crankshaft, acts as a flywheel[10]) store the potential energy. The moving masses of the pistons store the kinetic energy of the system.[11]

At this point, it is probably good to quickly review the relevant math. If the magnitude of the oscillation is equal to *a*, then the motion of the piston (or the mass on a spring) will be described by *x* = *a*Ā·cos(ĻĀ·t + Ī).[12] Needless to say, Ī is just a phase factor which defines our *t* = 0 point, and Ļ is the *natural angular *frequency of our oscillator. Because of the 90Ā° angle between the two cylinders, Ī would be 0 for one oscillator, and āĻ/2 for the other. Hence, the motion of one piston is given by *x* = *a*Ā·cos(ĻĀ·t), while the motion of the other is given by *x* = *a*Ā·cos(ĻĀ·tāĻ/2) = *a*Ā·sin(ĻĀ·t).

The kinetic and potential energy of *one *oscillator (think of one piston or one spring only) can then be calculated as:

- K.E. = T = mĀ·
*v*^{2}/2 = (1/2)Ā·mĀ·Ļ^{2}Ā·*a*^{2}Ā·sin^{2}(ĻĀ·t + Ī) - P.E. = U = kĀ·x
^{2}/2 = (1/2)Ā·kĀ·*a*^{2}Ā·cos^{2}(ĻĀ·t + Ī)

The coefficient k in the potential energy formula characterizes the restoring force: F = ākĀ·x. From the dynamics involved, it is obvious that k must be equal to mĀ·Ļ^{2}. Hence, the total energy is equal to:

E = T + U = (1/2)Ā· mĀ·Ļ^{2}Ā·*a*^{2}Ā·[sin^{2}(ĻĀ·t + Ī) + cos^{2}(ĻĀ·t + Ī)] = mĀ·*a*^{2}Ā·Ļ^{2}/2

To facilitate the calculations, we will briefly assume k = mĀ·Ļ^{2} and *a* are equal to 1. The *motion *of our first oscillator is given by the cos(ĻĀ·t) = cosĪø function (Īø = ĻĀ·t), and its kinetic energy will be equal to sin^{2}Īø. Hence, the (instantaneous) *change *in kinetic energy at any point in time will be equal to:

d(sin^{2}Īø)/dĪø = 2āsinĪøād(sinĪø)/dĪø = 2āsinĪøācosĪø

Let us look at the second oscillator now. Just think of the second piston going up and down in the V-2 engine. Its motion is given by the sinĪø function, which is equal to cos(ĪøāĻ /2). Hence, its kinetic energy is equal to sin^{2}(ĪøāĻ /2), and how it *changes *ā as a function of Īø ā will be equal to:

2āsin(ĪøāĻ /2)ācos(ĪøāĻ /2) = = ā2ācosĪøāsinĪø = ā2āsinĪøācosĪø

We have our *perpetuum mobile*! While transferring kinetic energy from one piston to the other, the crankshaft will rotate with a constant angular velocity: linear motion becomes circular motion, and vice versa, and the total energy that is stored in the system is T + U = m*a*^{2}Ļ^{2}.

We have a great *metaphor* here. Somehow, in this beautiful interplay between linear and circular motion, energy is borrowed from one place and then returns to the other, cycle after cycle. We know the wavefunction consist of a sine and a cosine: the cosine is the real component, and the sine is the imaginary component. Could they be equally real? Could each represent *half *of the total energy of our particle? Should we think of the *c *in our E = m*c*^{2} formula as an *angular *velocity?

These are sensible questions. Let us explore them.** **

# II. The wavefunction as a two-dimensional oscillation

The elementary wavefunction is written as:

Ļ = *aĀ·e*^{āi[EĀ·t ā pāx]/Ä§} = *aĀ·e*^{āi[EĀ·t ā pāx]/Ä§} = *aĀ·cos( pāx/Ä§ *

*–*

*Eāt/Ä§) + iĀ·aĀ·sin(*

**p**ā**x**/Ä§*–*

*Eāt/Ä§)*

*When *considering a particle at rest (**p** = **0**) this reduces to:

Ļ = *aĀ·e*^{āiāEĀ·t/Ä§} = *aĀ·cos(**–**Eāt/Ä§) + iĀ·aĀ·sin(**–**Eāt/Ä§) = aĀ·cos(Eāt/Ä§) **–** iĀ·aĀ·sin(Eāt/Ä§) *

Let us remind ourselves of the geometry involved, which is illustrated below. Note that the argument of the wavefunction rotates *clockwise *with time, while the mathematical convention for measuring the phase angle (Ļ) is *counter*-clockwise.

**Figure 2**: Eulerās formula

If we assume the momentum **p** is all in the *x*-direction, then the **p** and **x** vectors will have the same direction, and **p***ā x/Ä§ reduces to pāx/Ä§. Most illustrations ā such as the one below ā will either freeze x or, else, t. Alternatively, one can google web animations varying both. *The point is: we also have a two-dimensional oscillation here. These two dimensions are perpendicular to the direction of propagation of the wavefunction. For example, if the wavefunction propagates in the

*x*-direction, then the oscillations are along the

*y*– and

*z*-axis, which we may refer to as the real and imaginary axis. Note how the phase difference between the cosine and the sine ā the real and imaginary part of our wavefunction ā appear to give some spin to the whole. I will come back to this.

**Figure 3**: Geometric representation of the wavefunction

Hence, *if *we would say these oscillations carry half of the total energy of the particle, then we may refer to the real and imaginary energy of the particle respectively, and the interplay between the real and the imaginary *part of the wavefunction may then describe how energy propagates through space over time. *

Let us consider, once again, a particle at rest. Hence, **p** = **0** and the (elementary) wavefunction reduces to Ļ = *aĀ·e*^{āiāEĀ·t/Ä§}. Hence, the angular velocity of both oscillations, at some point **x**, is given by Ļ = -E/Ä§. Now, the energy of our particle includes all of the energy ā kinetic, potential and rest energy ā and is, therefore, equal to E = m*c*^{2}.

Can we, somehow, relate this to the mĀ·*a*^{2}Ā·Ļ^{2} energy formula for our V-2 *perpetuum mobile*? Our wavefunction has an amplitude too. Now, if the oscillations of the real and imaginary wavefunction store the energy of our particle, then their amplitude will surely matter. In fact, the energy of an oscillation is, in general, proportional to the *square *of the amplitude: E Āµ *a*^{2}. We may, therefore, think that the *a*^{2} factor in the E = mĀ·*a*^{2}Ā·Ļ^{2} energy will surely be relevant as well.

However, here is a complication: an *actual* particle is localized in space and can, therefore, *not *be represented by the elementary wavefunction. We must build a wave *packet* for that: a sum of wavefunctions, each with their own amplitude *a*_{k}, and their own Ļ* _{i}* = -E

*/Ä§. Each of these wavefunctions will*

_{i}*contribute*some energy to the total energy of the wave packet. To calculate the contribution of each wave to the total, both

*a*as well as E

_{i}*will matter.*

_{i}What is E* _{i}*? E

*varies around some average E, which we can associate with some*

_{i}*average mass*m: m = E/

*c*

^{2}. The Uncertainty Principle kicks in here. The analysis becomes more complicated, but a formula such as the one below might make sense:We can re-write this as:What is the meaning of this equation? We may look at it as some sort of

*physical*normalization condition when building up the

*Fourier sum*. Of course, we should relate this to the

*mathematical*normalization condition for the wavefunction. Our intuition tells us that the probabilities must be related to the energy

*densities*, but how exactly? We will come back to this question in a moment. Let us first think some more about the enigma:

**what**

*is*mass?Before we do so, let us quickly calculate the value of *c*^{2}Ä§^{2}: it is about 1Ā“10^{–}^{51} N^{2}ām^{4}. Let us also do a dimensional analysis: the physical dimensions of the E = mĀ·*a*^{2}Ā·Ļ^{2} equation make sense if we express m in kg, *a *in m, and Ļ in *rad*/s. We then get: [E] = kgām^{2}/s^{2} = (Nās^{2}/m)ām^{2}/s^{2} = Nām = J. The dimensions of the left- and right-hand side of the physical normalization condition is N^{3}ām^{5}.** **

# III. What is mass?

We came up, playfully, with a meaningful interpretation for energy: it is a two-dimensional oscillation of mass. But what is mass? A new *aether *theory is, of course, not an option, but then what *is* it that is oscillating? To understand the physics behind equations, it is always good to do an analysis of the physical dimensions in the equation. Let us start with Einsteinās energy equation once again. If we want to look at mass, we should re-write it as *m* = E/c^{2}:

[*m*] = [E/*c*^{2}] = J/(m/s)^{2} = NĀ·mās^{2}/m^{2} = NĀ·s^{2}/m = kg

This is not very helpful. It only reminds us of Newtonās definition of a mass: mass is that what gets accelerated by a force. At this point, we may want to think of the physical significance of the *absolute *nature of the speed of light. Einsteinās E = m*c*^{2} equation implies we can write the ratio between the energy and the mass of *any *particle is always the same, so we can write, for example:This reminds us of the Ļ^{2}= *C*^{–}^{1}/*L* or Ļ^{2} = *k*/*m* of harmonic oscillators once again.[13] The key difference is that the Ļ^{2}= *C*^{–}^{1}/*L* and Ļ^{2} = *k*/*m* formulas introduce *two *or more degrees of freedom.[14] In contrast, *c*^{2}= E/m for *any *particle, *always*. However, that is exactly the point: we can modulate the resistance, inductance and capacitance of electric circuits, and the stiffness of springs and the masses we put on them, but we live in *one *physical space only: *our *spacetime. Hence, the speed of light *c* emerges here as *the* defining property of spacetime ā the resonant frequency, so to speak. We have no further degrees of freedom here.

The Planck-Einstein relation (for photons) and the *de Broglie *equation (for matter-particles) have an interesting feature: both imply that the *energy *of the oscillation is proportional to the frequency, with Planckās constant as the constant of proportionality. Now, for *one-dimensional *oscillations ā think of a guitar string, for example ā we know the energy will be proportional to the *square *of the frequency. It is a remarkable observation: the two-dimensional matter-wave, or the electromagnetic wave, gives us *two* waves for the price of one, so to speak, each carrying *half* of the *total *energy of the oscillation but, as a result, we get a proportionality between E and *f* instead of between E and *f*^{2}.

However, such reflections do not answer the fundamental question we started out with: what *is *mass? At this point, it is hard to go beyond the circular definition that is implied by Einsteinās formula: energy is a two-dimensional oscillation of mass, and mass packs energy, and *c *emerges us as the property of spacetime that defines *how *exactly.

When everything is said and done, this does not go beyond stating that mass is some scalar field. Now, a scalar field is, quite simply, some real *number* that we associate with a position in spacetime. The Higgs field is a scalar field but, of course, the theory behind it goes much beyond stating that we should think of mass as some scalar field. The fundamental question is: why and how does energy, or matter, *condense *into elementary particles? That is what the Higgs *mechanism* is about but, as this paper is exploratory only, we cannot even start explaining the basics of it.

What we *can *do, however, is look at the wave *equation *again (SchrĆ¶dingerās equation), as we can now analyze it as an energy diffusion equation.** **

# IV. SchrĆ¶dingerās equation as an energy diffusion equation

The interpretation of SchrĆ¶dingerās equation as a diffusion equation is straightforward. Feynman (*Lectures*, III-16-1) briefly summarizes it as follows:

āWe can think of SchrĆ¶dingerās equation as describing the diffusion of the probability amplitude from one point to the next. [ā¦] But the imaginary coefficient in front of the derivative makes the behavior completely different from the ordinary diffusion such as you would have for a gas spreading out along a thin tube. Ordinary diffusion gives rise to real exponential solutions, whereas the solutions of SchrĆ¶dingerās equation are complex waves.ā[17]

Let us review the basic math. For a particle moving in free space ā with no external force fields acting on it ā there is no potential (U = 0) and, therefore, the UĻ term disappears. Therefore, SchrĆ¶dingerās equation reduces to:

āĻ(**x**, t)/āt = *i*Ā·(1/2)Ā·(Ä§/m_{eff})Ā·ā^{2}Ļ(**x**, t)

The ubiquitous diffusion equation in physics is:

āĻ(**x**, t)/āt = DĀ·ā^{2}Ļ(**x**, t)

The *structural* similarity is obvious. The key difference between both equations is that the wave equation gives us *two *equations for the price of one. Indeed, because Ļ is a complex-valued function, with a *real *and an *imaginary *part, we get the following equations[18]:

*Re*(āĻ/āt) = ā(1/2)Ā·(Ä§/m_{eff})Ā·*Im*(ā^{2}Ļ)*Im*(āĻ/āt) = (1/2)Ā·(Ä§/m_{eff})Ā·*Re*(ā^{2}Ļ)

These equations make us think of the equations for an electromagnetic wave in free space (no stationary charges or currents):

- ā
**B**/āt = āāĆ**E** - ā
**E**/āt =*c*^{2}āĆ**B**

The above equations effectively describe a *propagation *mechanism in spacetime, as illustrated below.

**Figure 4**: Propagation mechanisms

The Laplacian operator (ā^{2}), when operating on a *scalar *quantity, gives us a flux density, i.e. something expressed per square meter (1/m^{2}). In this case, it is operating on Ļ(**x**, t), so what is the dimension of our wavefunction Ļ(**x**, t)? To answer that question, we should analyze the diffusion constant in SchrĆ¶dingerās equation, i.e. the (1/2)Ā·(Ä§/m_{eff}) factor:

- As a
*mathematical*constant of proportionality, it will*quantify*the relationship between both derivatives (i.e. the time derivative and the Laplacian); - As a
*physical*constant, it will ensure the*physical dimensions*on both sides of the equation are compatible.

Now, the Ä§/m_{eff} factor is expressed in (NĀ·mĀ·s)/(NĀ· s^{2}/m) = m^{2}/s. Hence, it does ensure the dimensions on both sides of the equation are, effectively, the same: āĻ/āt is a time derivative and, therefore, its dimension is s^{–}^{1} while, as mentioned above, the dimension of ā^{2}Ļ is m^{–}^{2}. However, this does not solve our basic question: what is the dimension of the real and imaginary part of our wavefunction?

At this point, mainstream physicists will say: it does not have a physical dimension, and there is no geometric interpretation of SchrĆ¶dingerās equation. One may argue, effectively, that its argument, (**p**ā**x** – Eāt)/Ä§, is just a number and, therefore, that the real and imaginary part of Ļ is also just some number.

To this, we may object that Ä§ may be looked as a mathematical scaling constant only.** If **we do that,

**the argument of Ļ will, effectively, be expressed in**

*then**action*units, i.e. in NĀ·mĀ·s. It then does make sense to also associate a physical dimension with the real and imaginary part of Ļ. What could it be?

We may have a closer look at Maxwellās equations for inspiration here. The electric field vector is expressed in *newton* (the unit of force) per unit of *charge* (*coulomb*). Now, there is something interesting here. The physical dimension of the magnetic field is N/C *divided* by m/s.[19] We may write **B** as the following vector cross-product: **B** = (1/*c*)ā**e****_{x}**Ć

**E**, with

**e****the unit vector pointing in the**

_{x}*x*-direction (i.e. the direction of propagation of the wave). Hence, we may associate the (1/

*c*)ā

**e****Ć**

_{x}*operator*, which amounts to a rotation by 90 degrees, with the s/m dimension. Now, multiplication by

*i*also amounts to a rotation by 90Ā° degrees. Hence, we may boldly write:

**B**= (1/

*c*)ā

**e****Ć**

_{x}**E**= (1/

*c*)ā

*i*ā

**E**. This allows us to also geometrically interpret SchrĆ¶dingerās equation in the way we interpreted it above (see Figure 3).[20]

Still, we have not answered the question as to what the physical dimension of the real and imaginary part of our wavefunction should be. At this point, we may be inspired by the structural similarity between Newtonās and Coulombās force laws:Hence, if the electric field vector **E **is expressed in force per unit *charge *(N/C), then we may want to think of associating the real part of our wavefunction with a force per unit *mass* (N/kg). We can, of course, do a substitution here, because the mass unit (1 kg) is equivalent to 1 NĀ·s^{2}/m. Hence, our N/kg dimension becomes:

N/kg = N/(NĀ·s^{2}/m)= m/s^{2}

What is this: m/s^{2}? Is *that *the dimension of the *a*Ā·*cos*Īø term in the *a*Ā·*e*^{āiĪø }= *a*Ā·*cos*Īø ā *i*Ā·*a*Ā·*sin*Īø wavefunction?

My answer is: **why not?** Think of it: m/s^{2} is the physical dimension of *acceleration*: the increase or decrease in velocity (m/s) per second. It ensures the wavefunction for *any *particle ā matter-particles or particles with zero rest mass (photons) ā and the associated wave *equation *(which has to be the same for all, as the spacetime we live in is *one*) are mutually consistent.

In this regard, we should think of how we would model a *gravitational *wave. The physical dimension would surely be the same: force per mass unit. It all makes sense: wavefunctions may, perhaps, be interpreted as traveling distortions of spacetime, i.e. as tiny gravitational waves.

# V. Energy densities and flows

Pursuing the geometric equivalence between the equations for an electromagnetic wave and SchrĆ¶dingerās equation, we can now, perhaps, see if there is an equivalent for the energy density. For an electromagnetic wave, we know that the energy density is given by the following formula:**E** and **B** are the electric and magnetic field vector respectively. The Poynting vector will give us the directional energy flux, i.e. the energy flow per unit area per unit time. We write:Needless to say, the **ā**ā operator is the divergence and, therefore, gives us the magnitude of a (vector) fieldās *source* or *sink* at a given point. To be precise, the divergence gives us the volume density of the outward *flux *of a vector field from an infinitesimal volume around a given point. In this case, it gives us the *volume density* of the flux of ** S**.

We can analyze the dimensions of the equation for the energy density as follows:

**E**is measured in*newton per coulomb*, so [**E**ā**E**] = [E^{2}] = N^{2}/C^{2}.**B**is measured in (N/C)/(m/s), so we get [**B**ā**B**] = [B^{2}] = (N^{2}/C^{2})Ā·(s^{2}/m^{2}). However, the dimension of our*c*^{2}factor is (m^{2}/s^{2}) and so weāre also left with N^{2}/C^{2}.- The
*Ļµ*_{0}is the electric constant, aka as the vacuum permittivity. As a*physical*constant, it should ensure the dimensions on both sides of the equation work out, and they do: [Īµ_{0}] = C^{2}/(NĀ·m^{2}) and, therefore, if we multiply that with N^{2}/C^{2}, we find that*u*is expressed in J/m^{3}.[21]

Replacing the *newton per coulomb* unit (N/C) by the *newton per kg* unit (N/kg) in the formulas above should give us the equivalent of the energy density for the wavefunction. We just need to substitute *Ļµ*_{0} for an equivalent constant. We may to give it a try. If the energy densities can be calculated ā which are also mass densities, obviously ā then the probabilities should be proportional to them.

Let us first see what we get for a photon, assuming the electromagnetic wave represents its wavefunction. Substituting **B** for (1/*c*)ā*i*ā**E** or for ā(1/*c*)ā*i*ā**E** gives us the following result:**Zero!?** An unexpected result! Or not? We have no stationary charges and no currents: only an electromagnetic wave in free space. Hence, the local energy conservation principle needs to be respected at all points in space and in time. The geometry makes sense of the result: for an electromagnetic wave, the magnitudes of **E** and **B** reach their maximum, minimum and zero point *simultaneously*, as shown below.[22] This is because their *phase *is the same.

**Figure 5**: Electromagnetic wave: **E** and **B**

Should we expect a similar result for the energy densities that we would associate with the real and imaginary part of the matter-wave? For the matter-wave, we have a phase difference between *a*Ā·*cos*Īø and *a*Ā·*sin*Īø, which gives a different picture of the *propagation *of the wave (see Figure 3).[23] In fact, the geometry of the suggestion suggests some inherent spin, which is interesting. I will come back to this. Let us first guess those densities. Making abstraction of any scaling constants, we may write:We get what we hoped to get: the absolute square of our amplitude is, effectively, an energy density !

|Ļ|^{2 } = |*aĀ·e*^{āiāEĀ·t/Ä§}|^{2 }= *a*^{2 }= *u*

This is very deep. A photon has no rest mass, so it borrows and returns energy from empty space as it travels through it. In contrast, a matter-wave carries energy and, therefore, has some (*rest*) mass. It is therefore associated with an energy density, and this energy density gives us the probabilities. Of course, we need to fine-tune the analysis to account for the fact that we have a wave packet rather than a single wave, but that should be feasible.

As mentioned, the phase difference between the real and imaginary part of our wavefunction (a cosine and a sine function) appear to give some spin to our particle. We do not have this particularity for a photon. Of course, photons are bosons, i.e. spin-zero particles, while elementary matter-particles are fermions with spin-1/2. Hence, our geometric interpretation of the wavefunction suggests that, after all, there may be some more intuitive explanation of the fundamental dichotomy between bosons and fermions, which puzzled even Feynman:

āWhy is it that particles with half-integral spin are Fermi particles, whereas particles with integral spin are Bose particles? We apologize for the fact that we cannot give you an elementary explanation. An explanation has been worked out by Pauli from complicated arguments of quantum field theory and relativity. He has shown that the two must necessarily go together, but we have not been able to find a way of reproducing his arguments on an elementary level. It appears to be one of the few places in physics where there is a rule which can be stated very simply, but for which no one has found a simple and easy explanation. The explanation is deep down in relativistic quantum mechanics. This probably means that we do not have a complete understanding of the fundamental principle involved.ā (Feynman, *Lectures*, III-4-1)

The *physical* interpretation of the wavefunction, as presented here, may provide some better understanding of āthe fundamental principle involvedā:* the physical dimension of the oscillation is just very different*. That is all: it is force per unit charge for photons, and force per unit mass for matter-particles. We will examine the question of spin somewhat more carefully in section VII. Let us first examine the matter-wave some more.** **

# VI. Group and phase velocity of the matter-wave

The geometric representation of the matter-wave (see Figure 3) suggests a traveling wave and, yes, of course: the matter-wave effectively *travels* through space and time. But *what is traveling, exactly*? It is the pulse ā or the *signal *ā only: the *phase *velocity of the wave is just a mathematical concept and, even in our physical interpretation of the wavefunction, the same is true for the *group *velocity of our wave packet. The oscillation is two-dimensional, but perpendicular to the direction of travel of the wave. Hence, nothing actually moves *with *our particle.

Here, we should also reiterate that we did not answer the question as to *what *is oscillating up and down and/or sideways: we only associated a *physical *dimension with the components of the wavefunction ā *newton* per *kg* (force per unit mass), to be precise. We were inspired to do so because of the physical dimension of the electric and magnetic field vectors (*newton* per *coulomb*, i.e. force per unit charge) we associate with electromagnetic waves which, for all practical purposes, we currently treat as the wavefunction for a photon. This made it possible to calculate the associated *energy densities *and a *Poynting vector *for energy dissipation. In addition, we showed that SchrĆ¶dinger’s equation itself then becomes a diffusion equation for energy. However, let us now focus some more on the asymmetry which is introduced by the phase difference between the real and the imaginary part of the wavefunction. Look at the mathematical shape of the elementary wavefunction once again:

Ļ = *aĀ·e*^{āi[EĀ·t ā pāx]/Ä§} = *aĀ·e*^{āi[EĀ·t ā pāx]/Ä§} = *aĀ·cos*(**p**ā**x**/Ä§ ā Eāt/Ä§)* + iĀ·aĀ·sin*(**p**ā**x**/Ä§ ā Eāt/Ä§)

The minus sign in the argument of our sine and cosine function defines the direction of travel: an F(xā*vā*t) wavefunction will always describe some wave that is traveling in the *positive *x-direction (with *c *the wave velocity), while an F(x+*vā*t) wavefunction will travel in the *negative *x-direction. For a geometric interpretation of the wavefunction *in three dimensions*, we need to agree on how to define *i* or, what amounts to the same, a convention on how to define clockwise and counterclockwise directions: if we look at a clock from the back, then its hand will be moving *counter*clockwise. So we need to establish the equivalent of the right-hand rule. However, let us not worry about that now. Let us focus on the interpretation. To ease the analysis, we’ll assume we’re looking at a particle at rest. Hence, **p** = **0**, and the wavefunction reduces to:

Ļ = *aĀ·e*^{āiāEĀ·t/Ä§} = *aĀ·cos*(āEāt/Ä§)* + iĀ·aĀ·sin*(āE_{0}āt/Ä§)* = aĀ·cos*(E_{0}āt/Ä§) ā* iĀ·aĀ·sin*(E_{0}āt/Ä§)

E_{0} is, of course, the *rest *mass of our particle and, now that we are here, we should probably wonder *whose *time *t *we are talking about: is it *our* time, or is the proper time of our particle? Well… In this situation, we are both at rest so it does not matter: t *is*, effectively, the proper time so perhaps we should write it as t_{0}. It does not matter. You can see what we expect to see: E_{0}/Ä§ pops up as the *natural *frequency of our matter-particle: (E_{0}/Ä§)āt = Ļāt. Remembering the Ļ = 2ĻĀ·*f* = 2Ļ/T and T = 1/*f *formulas, we can associate a period and a frequency with this wave, using the Ļ = 2ĻĀ·*f* = 2Ļ/T. Noting that Ä§ = h/2Ļ, we find the following:

T = 2ĻĀ·(Ä§/E_{0}) = h/E_{0} ā *f *= E_{0}/h = m_{0}*c*^{2}/h

This is interesting, because we can look at the period as a *natural *unit of time for our particle. What about the wavelength? That is tricky because we need to distinguish between group and phase velocity here. The group velocity (*v*_{g}) should be zero here, because we assume our particle does not move. In contrast, the phase velocity is given by *v*_{p} = Ī»Ā·*f *= (2Ļ/k)Ā·(Ļ/2Ļ) = Ļ/k. In fact, we’ve got something funny here: the wavenumber k* = *p/Ä§ is zero, because we assume the particle is at rest, so p = 0. So we have a division by zero here, which is rather strange. What do we get assuming the particle is *not *at rest? We write:

*v*_{p} = Ļ/k = (E/Ä§)/(p/Ä§) = E/p = E/(mĀ·*v*_{g}) = (mĀ·*c*^{2})/(mĀ·*v*_{g}) = *c*^{2}/*v*_{g}

This is interesting: it establishes a reciprocal relation between the phase and the group velocity, with *c *as a simple scaling constant. Indeed, the graph below shows the *shape *of the function does *not *change with the value of *c*, and we may also re-write the relation above as:

*v*_{p}/*c *= Ī²_{p} = *c*/*v*_{p} = 1/Ī²_{g} = 1/(*c*/*v*_{p})

**Figure 6**: Reciprocal relation between phase and group velocity

We can also write the mentioned relationship as *v*_{p}Ā·*v*_{g} = *c*^{2}, which reminds us of the relationship between the electric and magnetic constant (1/Īµ_{0})Ā·(1/Ī¼_{0}) = *c*^{2}. This is interesting in light of the fact we can re-write this as (*c*Ā·Īµ_{0})Ā·(*c*Ā·Ī¼_{0}) = 1, which shows electricity and magnetism are just two sides of the same coin, so to speak.[24]

Interesting, but how do we interpret the math? What about the implications of the zero value for wavenumber k* = *p/Ä§. We would probably like to think it implies the elementary wavefunction should always be associated with *some *momentum, because the concept of zero momentum clearly leads to weird math: something times *zero *cannot be equal to *c*^{2}! Such interpretation is also consistent with the Uncertainty Principle: if ĪxĀ·Īp ā„ Ä§, then *neither* Īx *nor* Īp can be zero. In other words, the Uncertainty Principle tells us that the idea of a pointlike particle actually *being* at some *specific* point in time and in space does not make sense: it *has *to move. It tells us that our concept of dimensionless points in time and space are *mathematical *notions only. *Actual *particles – including photons – are always a bit spread out, so to speak, and – importantly – they *have to *move.

For a photon, this is self-evident. It has no rest mass, no rest energy, and, therefore, it is going to move at the speed of light itself. We write: p = mĀ·*c* = mĀ·*c*^{2}/*c *= E/*c*. Using the relationship above, we get:

*v*_{p} = Ļ/k = (E/Ä§)/(p/Ä§) = E/p = *c* ā *v*_{g} = *c*^{2}/*v*_{p} = *c*^{2}/*c* = *c*

This is good: we started out with some reflections on the *matter*-wave, but here we get an interpretation of the electromagnetic wave as a wavefunction for the photon. But let us get back to our matter-wave. In regard to our interpretation of a particle *having to *move, we should remind ourselves, once again, of the fact that an *actual* particle is always localized in space and that it can, therefore, *not *be represented by the elementary wavefunction Ļ = *aĀ·e*^{āi[EĀ·t ā pāx]/Ä§} or, for a particle at rest, the Ļ = *aĀ·e*^{āiāEĀ·t/Ä§} function. We must build a wave *packet* for that: a sum of wavefunctions, each with their own amplitude *a _{i}*, and their own Ļ

*= āE*

_{i}*/Ä§. Indeed, in section II, we showed that each of these wavefunctions will*

_{i}*contribute*some energy to the total energy of the wave packet and that, to calculate the contribution of each wave to the total, both

*a*as well as E

_{i}*matter. This may or may not resolve the apparent paradox. Let us look at the group velocity.*

_{i}To calculate a meaningful group velocity, we must assume the *v*_{g} = āĻ* _{i}*/āk

*= ā(E*

_{i}*/Ä§)/ā(p*

_{i}*/Ä§) = ā(E*

_{i}*)/ā(p*

_{i}*) exists. So we must have some*

_{i}*dispersion relation*. How do we calculate it? We need to calculate Ļ

*as a function of k*

_{i}

_{i}*here, or E*

_{ }*as a function of p*

_{i}*. How do we do that? Well… There are a few ways to go about it but one interesting way of doing it is to re-write SchrĆ¶dinger’s equation as we did, i.e. by distinguishing the real and imaginary parts of the āĻ/āt =*

_{i}*i*Ā·[Ä§/(2m)]Ā·ā

^{2}Ļ wave equation and, hence, re-write it as the following

*pair*of two equations:

*Re*(āĻ/āt) = ā[Ä§/(2m_{eff})]Ā·*Im*(ā^{2}Ļ) ā ĻĀ·cos(kx ā Ļt) = k^{2}Ā·[Ä§/(2m_{eff})]Ā·cos(kx ā Ļt)*Im*(āĻ/āt) = [Ä§/(2m_{eff})]Ā·*Re*(ā^{2}Ļ) ā ĻĀ·sin(kx ā Ļt) = k^{2}Ā·[Ä§/(2m_{eff})]Ā·sin(kx ā Ļt)

Both equations imply the following dispersion relation:

Ļ = Ä§Ā·k^{2}/(2m_{eff})

Of course, we need to think about the subscripts now: we have Ļ* _{i}*, k

*, but… What about m*

_{i}_{eff}or, dropping the subscript, m? Do we write it as m

*? If so, what is it? Well… It is the*

_{i}*equivalent*mass of E

*obviously, and so we get it from the mass-energy equivalence relation: m*

_{i}*= E*

_{i}*/*

_{i}*c*

^{2}. It is a fine point, but one most people forget about: they usually just write m. However, if there is uncertainty in the energy, then Einstein’s mass-energy relation tells us we must have some uncertainty in the (equivalent) mass too. Here, I should refer back to Section II: E

*varies around some*

_{i}*average*energy E and, therefore, the Uncertainty Principle kicks in.

# VII. Explaining spin

The elementary wavefunction *vector* ā i.e. the vector sum of the real and imaginary component ā rotates around the *x*-axis, which gives us the direction of propagation of the wave (see Figure 3). Its *magnitude *remains constant. In contrast, the magnitude of the electromagnetic vector ā defined as the vector sum of the electric and magnetic field vectors ā oscillates between zero and some maximum (see Figure 5).

We already mentioned that the *rotation *of the wavefunction vector appears to give some *spin* to the particle. Of course, a *circularly *polarized wave would also appear to have spin (think of the **E** and **B** vectors *rotating around* the direction of propagation – as opposed to oscillating up and down or sideways only). In fact, a circularly polarized light does carry angular momentum, as the *equivalent mass *of its energy may be thought of as rotating as well. But so here we are looking at a *matter*-wave.

The basic idea is the following: *if** *we look at Ļ =

*aĀ·e*

^{āiāEĀ·t/Ä§}as some

*real*vector ā as a two-dimensional oscillation of mass, to be precise ā

*then*we may associate its rotation around the direction of propagation with some torque. The illustration below reminds of the math here.

**Figure 7**: Torque and angular momentum vectors

A torque on some mass about a fixed axis gives it *angular momentum*, which we can write as the vector cross-product **L** = ** r**Ć

**p**or, perhaps easier for our purposes here as the product of an

*angular*velocity (

**Ļ**) and rotational inertia (I), aka as the

*moment of inertia*or the

*angular mass*. We write:

**L** = IĀ·**Ļ**

Note we can write **L** and **Ļ** in **boldface** here because they are (axial) vectors. If we consider their magnitudes only, we write L = IĀ·Ļ (no boldface). We can now do some calculations. Let us start with the angular velocity. In our previous posts, we showed that the *period *of the matter-wave is equal to T = 2ĻĀ·(Ä§/E_{0}). Hence, the angular velocity must be equal to:

Ļ = 2Ļ/[2ĻĀ·(Ä§/E_{0})] = E_{0}/Ä§

We also know the distance *r*, so that is the magnitude of *r** *in the **L** = * r*Ć

**p**vector cross-product: it is just

*a*, so that is the

*magnitude*of Ļ =

*aĀ·e*

^{āiāEĀ·t/Ä§}. Now, the momentum (

**p**) is the product of a

*linear*velocity (

*) – in this case, the*

**v***tangential*velocity – and some mass (m):

**p**= mĀ·

*. If we switch to*

**v***scalar*instead of vector quantities, then the (tangential) velocity is given by

*v*=

*r*Ā·Ļ. So now we only need to think about what we should use for m or, if we want to work with the

*angular*velocity (Ļ), the

*angular*mass (I). Here we need to make some assumption about the mass (or energy)

*distribution*. Now, it may or may not sense to assume the energy in the oscillation ā and, therefore, the mass ā is distributed uniformly. In that case, we may use the formula for the angular mass of a solid cylinder: I = mĀ·

*r*

^{2}/2. If we keep the analysis non-relativistic, then m = m

_{0}. Of course, the energy-mass equivalence tells us that m

_{0}= E

_{0}/

*c*

^{2}. Hence, this is what we get:

L = IĀ·Ļ = (m_{0}Ā·*r*^{2}/2)Ā·(E_{0}/Ä§) = (1/2)Ā·*a*^{2}Ā·(E_{0}/*c*^{2})Ā·(E_{0}/Ä§) = *a*^{2}Ā·E_{0}^{2}/(2Ā·Ä§Ā·*c*^{2})

Does it make sense? Maybe. Maybe not. Let us do a dimensional analysis: that wonāt check our logic, but it makes sure we made no mistakes when mapping mathematical and physical spaces. We have m^{2}Ā·J^{2} = m^{2}Ā·N^{2}Ā·m^{2} in the numerator and NĀ·mĀ·sĀ·m^{2}/s^{2} in the denominator. Hence, the dimensions work out: we get NĀ·mĀ·s as the dimension for L, which is, effectively, the physical dimension of angular momentum. It is also the *action *dimension, of course, and that cannot be a coincidence. Also note that the E = m*c*^{2} equation allows us to re-write it as:

L = *a*^{2}Ā·E_{0}^{2}/(2Ā·Ä§Ā·*c*^{2})

Of course, in quantum mechanics, we associate spin with the *magnetic *moment of a *charged* particle, not with its *mass *as such. Is there way to link the formula above to the one we have for the quantum-mechanical angular momentum, which is also measured in NĀ·mĀ·s units, and which can only take on one of two possible values: *J* = +Ä§/2 and āÄ§/2? It looks like a long shot, right? How do we go from (1/2)Ā·*a*^{2}Ā·m_{0}^{2}/Ä§ to Ā± (1/2)āÄ§? Let us do a numerical example. The energy of an electron is typically 0.510 MeV Ā» 8.1871Ć10^{ā14} Nām, and *a*ā¦ What value should we take for *a*?

We have an obvious *trio* of candidates here: the Bohr radius, the classical electron radius (aka the Thompon scattering length), and the Compton scattering radius.

Let us start with the Bohr radius, so that is about 0.Ć10^{ā10} Nām. We get L = *a*^{2}Ā·E_{0}^{2}/(2Ā·Ä§Ā·*c*^{2}) = 9.9Ć10^{ā31} Nāmās. Now that is about 1.88Ć10^{4} *times *Ä§/2. That is a *huge* factor. The Bohr radius cannot be right: we are *not *looking at an electron in an orbital here. To show it does not make sense, we may want to double-check the analysis by doing the calculation in another way. We said each oscillation will always pack 6.626070040(81)Ć10^{ā34} *joule *in energy. So our electron should pack about 1.24Ć10^{ā20} oscillations. The angular momentum (L) we get when using the Bohr radius for *a* and the value of 6.626Ć10^{ā34} *joule *for E_{0} and the Bohr radius is equal to 6.49Ć10^{ā59} Nāmās. So that is the angular momentum per oscillation. When we multiply this with the number of oscillations (1.24Ć10^{ā20}), we get about 8.01Ć10^{ā51} Nāmās, so that is a totally different number.

The classical electron radius is about 2.818Ć10^{ā15} m. We get an L that is equal to about 2.81Ć10^{ā39} Nāmās, so now it is a tiny *fraction *of Ä§/2! Hence, this leads us nowhere. Let us go for our last chance to get a meaningful result! Let us use the Compton scattering length, so that is about 2.42631Ć10^{ā12} m.

This gives us an L of 2.08Ć10^{ā33} Nāmās, which is only 20 times Ä§. This is not so bad, but it is good enough? Let us calculate it the other way around: what value should we *take *for *a *so as to ensure L = *a*^{2}Ā·E_{0}^{2}/(2Ā·Ä§Ā·*c*^{2}) = Ä§/2? Let us write it out:

In fact, this is the formula for the so-called *reduced *Compton wavelength. This is perfect. We found what we wanted to find. Substituting this value for *a *(you can calculate it: it is about 3.8616Ć10^{ā33} m), we get what we should find:

This is a rather spectacular result, and one that would ā a priori ā support the interpretation of the wavefunction that is being suggested in this paper.^{ }

# VIII. The boson-fermion dichotomy

Let us do some more thinking on the boson-fermion dichotomy. Again, we should remind ourselves that an *actual* particle is localized in space and that it can, therefore, *not *be represented by the elementary wavefunction Ļ = *aĀ·e*^{āi[EĀ·t ā pāx]/Ä§} or, for a particle at rest, the Ļ = *aĀ·e*^{āiāEĀ·t/Ä§} function. We must build a wave *packet* for that: a sum of wavefunctions, each with their own amplitude *a _{i}*, and their own Ļ

*= āE*

_{i}*/Ä§. Each of these wavefunctions will*

_{i}*contribute*some energy to the total energy of the wave packet. Now, we can have another wild but logical theory about this.

Think of the apparent right-handedness of the elementary wavefunction: surely, *Nature* can’t be bothered about our convention of measuring phase angles clockwise or counterclockwise. Also, the angular momentum can be positive or negative: *J* = +Ä§/2 or āÄ§/2. Hence, we would probably like to think that an actual particle – think of an electron, or whatever other particle you’d think of – may consist of right-handed as well as left-handed elementary waves. To be precise, we may think they *either *consist of (elementary) right-handed waves or, *else*, of (elementary) left-handed waves. An elementary right-handed wave would be written as:

Ļ(Īø* _{i}*)

*= a*Ā·(

_{i}*cos*Īø

*+*

_{i}*iĀ·sin*Īø

*)*

_{i}In contrast, an elementary left-handed wave would be written as:

Ļ(Īø* _{i}*)

*= a*Ā·(

_{i}*cos*Īø

*ā*

_{i}*iĀ·sin*Īø

*)*

_{i}How does that work out with the E_{0}Ā·t argument of our wavefunction? Position is position, and direction is direction, but time? Time has only one direction, but *Nature* surely does not care how we *count *time: counting like 1, 2, 3, etcetera or like ā1, ā2, ā3, etcetera is just the same. If we count like 1, 2, 3, etcetera, then we write our wavefunction like:

Ļ = *aĀ·cos*(E_{0}āt/Ä§)* ā iĀ·aĀ·sin*(E_{0}āt/Ä§)

If we count time like ā1, ā2, ā3, etcetera then we write it as:

Ļ = *aĀ·cos*(*ā*E_{0}āt/Ä§)* ā iĀ·aĀ·sin*(*ā*E_{0}āt/Ä§)= *aĀ·cos*(E_{0}āt/Ä§)* + iĀ·aĀ·sin*(E_{0}āt/Ä§)

Hence, it is just like the left- or right-handed circular polarization of an electromagnetic wave: we can have both for the matter-wave too! This, then, should explain why we can have *either *positive *or *negative quantum-mechanical spin (+Ä§/2 or āÄ§/2). It is the usual thing: we have two *mathematical *possibilities here, and so we *must *have two *physical *situations that correspond to it.

It is only natural. If we have left- and right-handed photons – or, generalizing, left- and right-handed bosons – then we should also have left- and right-handed fermions (electrons, protons, etcetera). Back to the dichotomy. The textbook analysis of the dichotomy between bosons and fermions may be epitomized by Richard Feynmanās *Lecture *on it (Feynman, III-4), which is confusing and ā I would dare to say ā even inconsistent: how are photons or electrons supposed to *know *that they need to interfere with a positive or a negative sign? They are not supposed to *know *anything: *knowledge *is part of our *interpretation *of whatever it is that is going on there.

Hence, it is probably best to keep it simple, and think of the dichotomy in terms of the different *physical *dimensions of the oscillation: newton per kg versus newton per coulomb. And then, of course, we should also note that matter-particles have a rest mass and, therefore, actually *carry* charge. Photons do not. But both are two-dimensional oscillations, and the point is: the so-called *vacuum *– and the *rest* *mass *of our particle (which is zero for the photon and non-zero for everything else) – give us the natural frequency for both oscillations, which is beautifully summed up in that remarkable equation for the group and phase velocity of the wavefunction, which applies to photons as well as matter-particles:

(*v _{phase}*Ā·

*c*)Ā·(

*v*Ā·

_{group}*c*) = 1 ā

*v*Ā·

_{p}*v*=

_{g}*c*

^{2}

The final question then is: why are photons spin-zero particles? Well… We should first remind ourselves of the fact that they do have spin when circularly polarized.[25] Here we may think of the rotation of the equivalent mass of their energy. However, if they are linearly polarized, then there is no spin. Even for circularly polarized waves, the spin angular momentum of photons is a weird concept. If photons have no (rest) mass, then they cannot carry any *charge*. They should, therefore, not have any *magnetic* moment. Indeed, what I wrote above shows an explanation of quantum-mechanical spin requires both mass *as well as *charge.[26]** **

# IX. Concluding remarks

There are, of course, other ways to look at the matter ā literally. For example, we can imagine two-dimensional oscillations as *circular *rather than linear oscillations. Think of a tiny ball, whose center of mass stays where it is, as depicted below. Any rotation ā around any axis ā will be some combination of a rotation around the two other axes. Hence, we may want to think of a two-dimensional oscillation as an oscillation of a polar and azimuthal angle.

**Figure 8**: Two-dimensional *circular *movement

The point of this paper is not to make any definite statements. That would be foolish. Its objective is just to challenge the simplistic mainstream viewpoint on the *reality *of the wavefunction. Stating that it is a mathematical construct only without *physical significance *amounts to saying it has no meaning at all. That is, clearly, a non-sustainable proposition.

The interpretation that is offered here looks at amplitude waves as traveling fields. Their physical dimension may be expressed in force per mass unit, as opposed to electromagnetic waves, whose amplitudes are expressed in force per (electric) *charge *unit. Also, the amplitudes of matter-waves incorporate a phase factor, but this may actually explain the rather enigmatic dichotomy between fermions and bosons and is, therefore, an added bonus.

The interpretation that is offered here has some advantages over other explanations, as it explains the *how *of diffraction and interference. However, while it offers a great explanation of the wave nature of matter, it does *not *explain its particle nature: while we think of the energy as being spread out, we will still *observe *electrons and photons as pointlike particles once they hit the detector. Why is it that a detector can sort of āhookā the whole blob of energy, so to speak?

The interpretation of the wavefunction that is offered here does *not *explain this. Hence, the *complementarity principle* of the Copenhagen interpretation of the wavefunction surely remains relevant.

# Appendix 1: The *de Broglie *relations and energy

The 1/2 factor in SchrĆ¶dingerās equation is related to the concept of the *effective *mass (m_{eff}). It is easy to make the wrong calculations. For example, when playing with the famous *de Broglie *relations ā aka as the matter-wave equations ā one may be tempted to *derive* the following energy concept:

- E = hĀ·
*f*and p = h/Ī». Therefore,*f*= E/h and Ī» = p/h. *v*=*fĀ·*Ī» = (E/h)ā(p/h) = E/p- p = mĀ·
*v*. Therefore, E =*v*Ā·p = mĀ·*v*^{2}

E = mĀ·*v*^{2}? This *resembles *the E = m*c*^{2} equation and, therefore, one may be enthused by the discovery, especially because the mĀ·*v*^{2} also pops up when working with the Least Action Principle in *classical *mechanics, which states that the path that is followed by a particle will minimize the following integral:Now, we can choose any reference point for the potential energy but, to reflect the energy conservation law, we can select a reference point that ensures the *sum* of the kinetic and the potential energy is zero *throughout *the time interval. If the force field is uniform, then the integrand will, effectively, be equal to KE ā PE *= mĀ·v*^{2}.[27]

However, that is *classical *mechanics and, therefore, not so relevant in the context of the *de Broglie *equations, and the apparent paradox should be solved by distinguishing between the *group *and the *phase *velocity of the matter wave.

# Appendix 2: The concept of the effective mass

The effective mass ā as used in SchrĆ¶dingerās equation ā is a rather enigmatic concept. To make sure we are making the right analysis here, I should start by noting you will usually see SchrĆ¶dingerās equation written as:This formulation includes a term with the potential energy (U). In free space (no potential), this term disappears, and the equation can be re-written as:

āĻ(**x**, t)/āt = *i*Ā·(1/2)Ā·(Ä§/m_{eff})Ā·ā^{2}Ļ(**x**, t)

We just moved the *i*Ā·Ä§ coefficient to the other side, noting that 1/*i *= –*i*. Now, in one-dimensional space, and assuming Ļ is just the elementary wavefunction (so we substitute *aĀ·e*^{āiā[EĀ·t ā pāx]/Ä§} for Ļ), this implies the following:

ā*a*Ā·*i*Ā·(E/Ä§)Ā·*e*^{ā}*iā*^{[EĀ·t ā pāx]/Ä§} = ā*i*Ā·(Ä§/2m_{eff})Ā·*a*Ā·(p^{2}/Ä§^{2})Ā·* e*^{āiā[EĀ·t ā pāx]/Ä§ }

ā E = p^{2}/(2m_{eff}) ā m_{eff} = mā(*v/c*)^{2}/2 = māĪ²^{2}/2

It is an ugly formula: it *resembles *the kinetic energy formula (K.E. = mā*v*^{2}/2) but it is, in fact, something completely different. The Ī²^{2}/2 factor ensures the *effective *mass is always a fraction of the mass itself. To get rid of the ugly 1/2 factor, we may re-define m_{eff} as *two *times the old m_{eff} (hence, m_{eff}^{NEW} = 2ām_{eff}^{OLD}), as a result of which the formula will look somewhat better:

m_{eff} = mā(*v/c*)^{2} = māĪ²^{2}

We know Ī² varies between 0 and 1 and, therefore, m_{eff} will vary between 0 and m. Feynman drops the subscript, and just writes m_{eff} as m in his textbook (see Feynman, III-19). On the other hand, the electron mass as used is also the electron mass that is used to calculate the size of an atom (see Feynman, III-2-4). As such, the two mass concepts are, effectively, mutually compatible. It is confusing because the same mass is often defined as the mass of a *stationary *electron (see, for example, the article on it in the online Wikipedia encyclopedia[28]).

In the context of the derivation of the electron orbitals, we do have the potential energy term ā which is the equivalent of a *source *term in a diffusion equation ā and that may explain why the above-mentioned m_{eff} = mā(*v/c*)^{2} = māĪ²^{2} formula does not apply.

# References

This paper discusses general principles in physics only. Hence, references can be limited to references to physics textbooks only. For ease of reading, any reference to additional material has been limited to a more popular undergrad textbook that can be consulted online: Feynmanās Lectures on Physics (http://www.feynmanlectures.caltech.edu). References are per volume, per chapter and per section. For example, Feynman III-19-3 refers to Volume III, Chapter 19, Section 3.

# Notes

[1] Of course, an *actual* particle is localized in space and can, therefore, *not *be represented by the elementary wavefunction Ļ = *aĀ·e*^{āiāĪø} = *aĀ·e*^{āi[EĀ·t ā pāx]/Ä§} = *aĀ·(cosĪø **–** iĀ·aĀ·sinĪø).* We must build a wave *packet* for that: a sum of wavefunctions, each with its own amplitude *a*_{k} and its own argument Īø_{k} = (E_{k}āt – **p**_{k}ā**x**)/Ä§. This is dealt with in this paper as part of the discussion on the mathematical and physical interpretation of the normalization condition.

[2] The N/kg dimension immediately, and naturally, reduces to the dimension of acceleration (m/s^{2}), thereby facilitating a direct interpretation in terms of Newtonās force law.

[3] In physics, a two-*spring *metaphor is more common. Hence, the pistons in the authorās *perpetuum mobile *may be replaced by springs.

[4] The author re-derives the equation for the Compton scattering radius in section VII of the paper.

[5] The magnetic force can be analyzed as a relativistic effect (see Feynman II-13-6). The dichotomy between the electric force as a polar vector and the magnetic force as an axial vector disappears in the relativistic four-vector representation of electromagnetism.

[6] For example, when using SchrĆ¶dingerās equation in a central field (think of the electron around a proton), the use of polar coordinates is recommended, as it ensures the symmetry of the Hamiltonian under all rotations (see Feynman III-19-3)

[7] This sentiment is usually summed up in the apocryphal quote: āGod does not play dice.āThe actual quote comes out of one of Einsteinās private letters to Cornelius Lanczos, another scientist who had also emigrated to the US. The full quote is as follows: “You are the only person I know who has the same attitude towards physics as I have: belief in the comprehension of reality through something basically simple and unified… It seems hard to sneak a look at God’s cards. But that He plays dice and uses ‘telepathic’ methods… is something that I cannot believe for a single moment.” (Helen Dukas and Banesh Hoffman, Albert Einstein, the Human Side: New Glimpses from His Archives, 1979)

[8] Of course, both are different velocities: Ļ is an *angular *velocity, while *v *is a *linear *velocity: Ļ is measured in *radians* per second, while *v *is measured in meter per second. However, the definition of a radian implies radians are measured in distance units. Hence, the physical dimensions are, effectively, the same. As for the formula for the total energy of an oscillator, we should actually write: E = mĀ·*a*^{2}āĻ^{2}/2. The additional factor (*a*) is the (maximum) amplitude of the oscillator.

[9] We also have a 1/2 factor in the E = m*v*^{2}/2 formula. Two remarks may be made here. First, it may be noted this is a non-relativistic formula and, more importantly, incorporates kinetic energy only. Using the Lorentz factor (Ī³), we can write the relativistically correct formula for the kinetic energy as K.E. = E ā E_{0} = m_{v}*c*^{2} ā m_{0}*c*^{2} = m_{0}Ī³*c*^{2} ā m_{0}*c*^{2} = m_{0}*c*^{2}(Ī³ ā 1). As for the *exclusion *of the potential energy, we may note that we may choose our reference point for the potential energy such that the kinetic and potential energy *mirror *each other. The energy concept that then emerges is the one that is used in the context of the Principle of Least Action: it equals E = m*v*^{2}. Appendix 1 provides some notes on that.

[10] Instead of two cylinders with pistons, one may also think of connecting two springs with a crankshaft.

[11] It is interesting to note that we may look at the energy in the rotating flywheel as *potential *energy because it is energy that is associated with motion, albeit *circular *motion. In physics, one may associate a rotating object with kinetic energy using the rotational equivalent of mass and linear velocity, i.e. *rotational inertia* (I) and angular velocity Ļ. The *kinetic *energy of a rotating object is then given by K.E. = (1/2)Ā·IĀ·Ļ^{2}.

[12] Because of the sideways motion of the connecting rods, the sinusoidal function will describe the linear motion only *approximately**,* but you can easily imagine the idealized limit situation.

[13] The Ļ^{2}= 1/*LC formula gives us the natural or resonant frequency for a electric circuit consisting of a resistor (R), an inductor (L), and a capacitor (C). Writing the formula as *Ļ^{2}= *C*^{–}^{1}/*L introduces the concept of elastance, which is the equivalent of the mechanical stiffness (k) of a spring.*

[14] The resistance in an electric circuit introduces a damping factor. When analyzing a mechanical spring, one may also want to introduce a drag coefficient. Both are usually defined as a fraction of the *inertia*, which is the mass for a spring and the inductance for an electric circuit. Hence, we would write the resistance for a spring as Ī³*m* and as R = Ī³*L* respectively.

[15] Photons are emitted by atomic oscillators: atoms going from one state (energy level) to another. Feynman (*Lectures*, I-33-3) shows us how to calculate the Q of these atomic oscillators: it is of the order of 10^{8}, which means the wave train will last about 10^{ā8 }seconds (to be precise, that is the time it takes for the radiation to die out by a factor 1/*e*). For example, for sodium light, the radiation will last about 3.2Ć10^{ā8 }seconds (this is the so-called decay time Ļ). Now, because the frequency of sodium light is some 500 THz (500Ć10^{12 }oscillations per second), this makes for some 16 million oscillations. There is an interesting paradox here: the speed of light tells us that such wave train will have a length of about 9.6 m! How is that to be reconciled with the pointlike nature of a photon? The paradox can only be explained by relativistic length contraction: in an analysis like this, one need to distinguish the reference frame of the photon ā riding along the wave as it is being emitted, so to speak ā and our stationary reference frame, which is that of the emitting atom.

[16] This is a general result and is reflected in the K.E. = T = (1/2)Ā·mĀ·Ļ^{2}Ā·*a*^{2}Ā·sin^{2}(ĻĀ·t + Ī) and the P.E. = U = kĀ·x^{2}/2 = (1/2)Ā· mĀ·Ļ^{2}Ā·*a*^{2}Ā·cos^{2}(ĻĀ·t + Ī) formulas for the linear oscillator.

[17] Feynman further formalizes this in his *Lecture on Superconductivity *(Feynman, III-21-2), in which he refers to SchrĆ¶dingerās equation as the āequation for continuity of probabilitiesā. The analysis is centered on the *local *conservation of energy, which confirms the interpretation of SchrĆ¶dingerās equation as an energy diffusion equation.

[18] The m_{eff} is the *effective* mass of the particle, which depends on the medium. For example, an electron traveling in a solid (a transistor, for example) will have a different effective mass than in an atom. In free space, we can drop the subscript and just write m_{eff} = m. Appendix 2 provides some additional notes on the concept. As for the equations, they are easily derived from noting that two complex numbers a + *i*āb and c + *i*ād are equal if, and only if, their real and imaginary parts are the same. Now, the āĻ/āt = *i*ā(Ä§/m_{eff})āā^{2}Ļ equation amounts to writing something like this: a + *i*āb = *i*ā(c + *i*ād). Now, remembering that *i*^{2} = ā1, you can easily figure out that *i*ā(c + *i*ād) = *i*āc + *i*^{2}ād = ā d + *i*āc.

[19] The dimension of **B** is usually written as N/(māA), using the SI unit for current, i.e. the *ampere *(A). However, 1 C = 1 Aās and, hence, 1 N/(māA) = 1 (N/C)/(m/s). * *

[20] Of course, multiplication with* i *amounts to a *counter*clockwise rotation. Hence, multiplication by –*i* also amounts to a rotation by 90 degrees, but *clockwise*. Now, to uniquely identify the clockwise and counterclockwise directions, we need to establish the equivalent of the right-hand rule for a proper geometric interpretation of SchrĆ¶dingerās equation in three-dimensional space: if we look at a clock from the back, then its hand will be moving *counter*clockwise. When writing **B** = (1/*c*)ā*i*ā**E**, we assume we are looking in the *negative x*-direction. If we are looking in the positive *x*-direction, we should write: **B** = -(1/*c*)ā*i*ā**E**. Of course, Nature does not care about our conventions. Hence, both should give the same results in calculations. We will show in a moment they do.

[21] In fact, when multiplying C^{2}/(NĀ·m^{2}) with N^{2}/C^{2}, we get N/m^{2}, but we can multiply this with 1 = m/m to get the desired result. It is significant that an energy density (*joule *per unit *volume*) can also be measured in *newton *(force per unit *area*.

[22] The illustration shows a linearly polarized wave, but the obtained result is general.

[23] The sine and cosine are essentially the same functions, except for the difference in the phase: sinĪø = cos(ĪøāĻ /2).

[24] I must thank a physics blogger for re-writing the 1/(Īµ_{0}Ā·Ī¼_{0}) = *c*^{2} equation like this. See: http://reciprocal.systems/phpBB3/viewtopic.php?t=236 (retrieved on 29 September 2017).

[25] A circularly polarized electromagnetic wave may be analyzed as consisting of two perpendicular electromagnetic plane waves of equal amplitude and 90Ā° difference in phase.

[26] Of course, the reader will now wonder: what about neutrons? How to explain neutron spin? Neutrons are neutral. That is correct, but neutrons are not elementary: they consist of (charged) quarks. Hence, neutron spin can (or should) be explained by the spin of the underlying quarks.

[27] We detailed the mathematical framework and detailed calculations in the following online article: https://readingfeynman.org/2017/09/15/the-principle-of-least-action-re-visited.

[28] https://en.wikipedia.org/wiki/Electron_rest_mass (retrieved on 29 September 2017).

# Light and matter

In my previous post, I discussed theĀ *de BroglieĀ *wave of a photon. It’s usually referred to as ** ‘the’** wave function (or the

*psi*function) but, as I explained, for every

*psi*– i.e. the position-space wave function ĪØ(

**x**,t) – there is also aĀ

*phi*Ā – i.e. the momentum-space wave function Ī¦(

**p**, t).

In that post, I alsoĀ *compared *itĀ – without much formalism – to theĀ *de BroglieĀ *wave of ‘matter particles’. Indeed, in physics, we look at ‘stuff’ as being made of particles and, while the taxonomy of *theĀ particle zoo* of the *Standard ModelĀ *of physics is rather complicated, one ‘taxonomic’ principle stands out: particles are * eitherĀ *matter particles (known as

*fermions*)

**force carriers (known as**

*or**bosons*). It’s a strict separation: either/or. No split personalities.

**A quick overview before we start…**

Wikipedia’s overview of particles in the Standard Model (including the latest addition: the Higgs boson) illustrates this fundamental dichotomy in nature: we have the matter particles (quarks and leptons) on one side, and the bosons (i.e. the force carriers) on the other side.

Don’t be put off by my remark on theĀ *particle zoo*: it’s a term coined in the 1960s, when the situation was quite confusing indeed (like more than *400* ‘particles’). However, the picture is quite orderly now. In fact, the *Standard ModelĀ *put an end to the discovery of ‘new’ particles, and it’s been stable since the 1970s, as experiments confirmed the reality of quarks. Indeed, all resistance to Gell-Man’s quarks and his flavor and color concepts – which are just words to describe new types of ‘charge’ – similar to electric charge but with more variety), ended when experiments by Stanford’s Linear Accelerator Laboratory (SLAC) in November 1974Ā confirmed the existence of the (second-generation and, hence, *heavy and unstable*)Ā ‘charm’ quark (again, the names suggest some frivolity but it’s serious physical research).

As for the Higgs boson, its existence of the Higgs boson had also been predicted, since 1964 to be precise, but it took fifty years to confirm it experimentally because only something like theĀ *Large Hadron ColliderĀ *could produce the required energy to find it in these particle smashing experiments – a rather crude way of analyzing matter, you may think, but so be it. [In case you harbor doubts on the Higgs particle, please note that, while CERN is the first to admit further confirmation is needed, the *Nobel Prize Committee*Ā apparently found the evidence ‘evidence enough’ to finally award Higgs and others a Nobel Prize for their ‘discovery’ fifty years ago – and, as you know, the Nobel Prize committee members are usually rather conservative in their judgment. So you would have to come up with a rather complex conspiracy theory to *denyĀ *its existence.]

Also note that theĀ *particle zooĀ *is actually less complicated than it looks at first sight: the (composite) particles that areĀ *stableĀ *in our world – *this *world –Ā consist of three quarks only: a proton consists of two up quarks and one down quark and, hence, is written as *uud*., and a neutron is two down quarks and one up quark:* udd*. Hence, **for all practical purposes** (i.e. for our discussion how light interacts with matter), **only the so-called first generation of matter-particles** – so that’s the first column in the overview above – are relevant.

All the particles in the second and third column are *unstable*. That being said, they survive long enough – a *muon* disintegrates after *2.2 millionths of a second* (on average) – to deserve the ‘particle’ title, as opposed to a ‘resonance’, whose lifetime can be as short as *a billionth of a trillionth of a second* – but we’ve gone through these numbers before and so I won’t repeat that here. Why do we need them? Well… We don’t, but they are a by-product of our world view (i.e. the Standard Model) and, for some reason, we find everything what this Standard Model says should exist, even if most of the stuff (all second- and third-generation matter particles, and all these *resonances*, vanish rather quickly – but so that also seems to be consistent with the model). [As for a possible fourth (or higher) generation, Feynman didn’t exclude it when he wrote his 1985 *Lectures* on quantum electrodynamics, but, checking on Wikipedia, I find the following: “According to the results of the statistical analysis by researchers from CERN and the Humboldt University of Berlin,Ā the existence of further fermions can be excluded with a probability of 99.99999% (5.3 sigma).” If you want to know why… Well… Read the rest of the Wikipedia article. It’s got to do with the Higgs particle.]

As for the (first-generation) **neutrino** in the table – the only one which you may not be familiar with – these are very spooky things but – I don’t want to scare you – relatively high-energy neutrinos are going through your and myĀ my body,Ā *right now and here,Ā *at a rate of some *hundred trillion per second*. They are produced by stars (stars are huge nuclear fusion reactors, remember?), and also as a by-product of these high-energy collisions in particle accelerators of course. But they are very hard to detect: the first *trace* of their existence was found in 1956 only – 26 years after their existence had been postulated: the fact that Wolfgang Pauli proposed their existence in 1930 to explain how beta decay could conserve energy, momentum and spin (angular momentum) demonstrates not only the genius but also the confidence of these early theoretical quantum physicists. Most neutrinos passing through Earth are produced by our Sun. Now they are being analyzed more routinely. The largestĀ *neutrino detectorĀ *on Earth is calledĀ *IceCube*. It sits on the South Pole ā orĀ *underĀ *it, as itās suspendedĀ *underĀ *the Antarctic ice, and it regularly capturesĀ high-energy neutrinos in the range of 1 to 10 TeV.Ā

Let me – to conclude this introduction – just quickly list and explain the *bosonsĀ *(i.e the force carriers) in the table above:

**1.** Of all of the bosons, the * photonĀ *(i.e. the topic of this post), is the most straightforward: there is onlyĀ

*typeĀ*of photon, even if it comes in different possible states of polarization.

[…]

I should probably do a quick note on polarization here – even if all of the stuff that follows will make abstraction of it. Indeed, the discussion on photons that follows (largely adapted from Feynman’s 1985 *Lectures on Quantum Electrodynamics*) assumes that there is no such thing as polarization – because it would make everything even more complicated.Ā The concept of polarization (linear, circular or elliptical) has a *direct *physical interpretation in classical mechanics (i.e. light as an electromagnetic wave). In quantum mechanics, however, polarization becomes a so-calledĀ *qubit *(quantum bit): leaving aside so-called *virtual photons *(these are short-range *disturbances *going between a proton and an electron in an atom – effectively mediating the electromagnetic force between them), the property of polarization comes in two basis states (0 and 1, or left and right), but these two basis states can be *superposed*. In *ket* notation: if Ā¦0āŖ and Ā¦1āŖ are the basis states, then any linear combination Ī±Ā·Ā¦0āŖ + ĆĀ·Ā¦1āŖ is also a valid state providedāĪ±ā^{2 }+Ā āĪ²ā^{2Ā }= 1, in line with the need to get probabilities that add up to one.

In case you wonder why I am introducing these *kets**, *there is no reason for it, except that I will be introducing some other tools in this post – such as Feynman diagrams – and so that’s all. In order to wrap this up, I need to note that *ketsĀ *are used in conjunction withĀ *bras*. So we have a bra-ket notation: the ket gives the starting condition, and the bra – denoted as ā©Ā Ā¦ – gives the final condition. They are combined in statements such as ā© particle arrives at *x*Ā¦particle leaves from *s*āŖ or – in short – ā© *x*Ā¦*s*āŖ and, while x and s would have some real-number value, ā©Ā *x*Ā¦*s*āŖ would denote the (complex-valued) probability amplitude associated wit the event consisting of these two conditions (i.e the starting and final condition).

But don’t worry about it. This digression is just what it is: a digression. Oh… Just make a mental note that the so-calledĀ *virtual* photons (the mediators that are supposed to keep the electron in touch with the proton) have *four* possible states of polarization – instead of two. They are related to the *fourĀ *directions of space (x, y and z) and time (t). š

**2. Gluons**, the exchange particles for the strong force, are more complicated: they come in eight so-calledĀ *colors.*Ā In practice, one should think of these colors as different *charges*, but so we have *more elementary chargesĀ *in this caseĀ than just plus or minus one (Ā±1) – as we have for the electric charge. So it’s just another type ofĀ *qubitĀ *in quantum mechanics.

[Note that the so-called *elementary* Ā±1 values for *electric* charge areĀ notĀ *really* elementary: it’s ā1/3 (for the *downĀ *quark,Ā and for the second- and third-generation *strange* and *bottom* quarks as well) and +2/3 (for the *up *quark as well as for the second- and third-generation charm and top quarks). That being said, electric charge takes two values only, and the Ā±1 value is easily found from a linear combination of the ā1/3 and +2/3 values.]

**3. Z and W bosons** carry the so-called weak force, aka as Fermiās interaction: they explain how one type of quark can change into another, thereby explaining phenomena such asĀ *beta*Ā *decay*. Beta decay explains why carbon-14 will, after a *very* long time (as compared to the ‘unstable’ particles mentioned above),Ā spontaneously decay into nitrogen-14. Indeed, carbon-12 is the (very) stable isotope, whileĀ carbon-14 has a life-time of 5,730 Ā± 40 years ‘only’Ā (so one can’t call carbon-12 ‘unstable’: perhaps ‘less stable’ will do)Ā and, hence, measuring how much carbon-14 is left in some organic substance allows us to date it (that’s what (radio)carbon-dating is about). As for the name, aĀ *betaĀ particle* can refer to an electronĀ *orĀ *a positron, so we can haveĀ *Ī²*^{āĀ }decay (e.g. the above-mentioned carbon-14 decay) as well as *Ī²*^{+Ā }decay (e.g. magnesium-23 into sodium-23). There’s also alpha and gamma decay but that involves different things.Ā

As you can see from the table, W^{Ā±Ā }and Z^{0Ā }bosons are *veryĀ *heavy (157,000 and 178,000 times heavier than a electron!), and W^{Ā± }carry the (positive or negative) electric charge. So why don’t we *see* them? Well… They are so short-lived that we can only see a tiny decay* width*, just a very tiny little *trace*,Ā so they resemble resonances in experiments. That’s also the reason why we see little or nothing of the weak force in real-life: the force-carrying particles mediating this force don’t get anywhere.

**4.** Finally, as mentioned above, theĀ **Higgs particle**Ā – and, hence, of the associated Higgs field ā had been predicted since 1964 already but its *existence* was only (tentatively)Ā *experimentally*Ā confirmed last year. The Higgs field gives fermions, and also the WĀ and ZĀ bosons, mass (but not photons and gluons), and – as mentioned above – thatās why the weak force has such short range as compared to the electromagnetic and strong forces. Note, however, that theĀ Higgs particle does actuallyĀ *notĀ *explain the gravitational force, so itāsĀ *not*Ā the (theoretical) graviton and there is *no *quantum field theory for the gravitational force as yet. JustĀ *GoogleĀ *it and you’ll quickly find out why: there’s theoretical as well as practical (experimental) reasons for that.

The Higgs field stands out from the other force fields because it’s a *scalarĀ *field (as opposed to a vector field). However, I have no idea how this so-called *Higgs mechanism*Ā (i.e. the interaction with matter particles (i.e. with the quarks and leptons, but *not *directly with neutrinos it would seem from the diagram below), with W and Z bosons, *and with itself *– but not with the massless photons and gluons) *actually works*. But then I still have aĀ *veryĀ *long way to go on thisĀ *Road to Reality*.

**In any case…Ā *** The topic of this post is to discuss light and its interaction with matter* – not the weak or strong force, nor the Higgs field.

Let’s go for it.

**Amplitudes, probabilities and observable properties**

Being born a boson *orĀ *a fermionĀ makes a big difference. That being said, both fermions and bosons areĀ *waviclesĀ *described by a complex-valuedĀ *psiĀ *function, colloquially known as the wave function. To be precise, there will be several wave functions, and the square of their modulus (sorry for the jargon) will give you the probability of someĀ *observable property* having a value in some relevant range, usually denoted by Ī. [I also explained (in my post on *Bose and Fermi*) how the rules forĀ *combiningĀ *amplitudes differ for bosons versus fermions, and how that explains why they are what they are: matter particles occupy space, while photons not onlyĀ *canĀ *but alsoĀ *likeĀ *to crowd together in, for example, a powerful laser beam. I’ll come back on that.]

For all practical purposes, relevant usually means ‘small enough to be meaningful’. For example, we may want to calculate the probability of detecting an electron in some tiny spacetime interval (Ī**x**,Ā Īt). [Again, ‘tiny’ in this context means small enough to be relevant: if we are looking at a hydrogen atom (whose size is a few *nano*meter), then Ī**x** is likely to be a cube or a sphere with an edge or a radius of a few *pico*meter only (a picometer is aĀ *thousandthĀ *of a nanometer, so it’s a millionth of a millionth of a meter); and, noting that the electron’s speed is approximately 2200 km *per second*… Well… I will letĀ *youĀ *calculate a relevant Īt. :-)]

If we want to do that, then we will need to square the modulus of the correspondingĀ *wave function* ĪØ(x, t). To be precise, we will have to do a *summationĀ *of all the values āĪØ(x, t)ā^{2Ā }over the interval and, because x and t are real (and, hence, continuous) numbers, that means doing some integral (because an integral is the continuous version of a sum).

But that’s only *one* example of an *observable property*: position. There are others. For example, we may not be interested in the particle’sĀ *exact *position but only in its momentum or energy. Well, we have another wave function for that: the *momentum* wave function Ī¦(x ,t). In fact, if you looked at my previous posts, you’ll remember the two are related because they are conjugate variables: Fourier transforms duals of one another. A less formal way of expressing that is to refer to the uncertainty principle. But this is not the time to repeat things.

The bottom line is that all particles travel through spacetime with a backpack full of complex-valued wave functions. We don’t know who and where these particles are exactly, and so weĀ can’t talk to them – but we can e-mail God and He’ll send us the wave function that we need to calculate some probability we are interested in because we want to check – in all kinds of experiments designed to fool them – if it matches with reality.

As mentioned above, I highlighted the main difference between bosons and fermions in myĀ *Bose and FermiĀ *post, so I won’t repeat that here. Just note that, when it comes to working with those probabilityĀ *amplitudesĀ *(that’s just another word for these *psi* and *phi*Ā functions), it makes aĀ *hugeĀ *difference: fermions and bosons interactĀ *veryĀ *differently. Bosons are *party* particles: they like to crowd and will always welcome an extra one. Fermions, on the other hand, will exclude each other: that’s why there’s something referred to as the *Fermi exclusion principleĀ *in quantum mechanics. That’s why fermions make matter (matter needs space) and bosons are force carriers (they’ll just call friends to help when the load gets heavier).

**Light versus matter: Quantum Electrodynamics**

OK. Let’s get down to business. This post is about light, or about light-matterĀ *interaction*. Indeed, in my previous post (on *Light*), IĀ promised to say something about the amplitude of a photon to go from point A to B (because – as I wrote in my previous post – that’s more ‘relevant’, when it comes to explaining stuff, than the amplitude of a photon to actually *beĀ *at point x at time t), and so that’s what I will do now.

In his 1985 *Lectures on Quantum ElectrodynamicsĀ *(which are lectures for the lay audience), Feynman writes the amplitude of a photon to go from point A to B as **P(A to B)** – and the P stands for ** p**hoton obviously,

*not*for

*p*robability. [I am tired of repeating that you need to square the modulus of an amplitude to get a probability but – here you are – I have said it once more.] That’s in line with the other

*fundamental*wave function in quantum electrodynamics (QED): the amplitude of an electron to go from A to B, which is written as

**E(A to B)**. [You got it: E just stands for

**lectron, not for our electric field vector.]**

*e*I also talked about the *thirdĀ *fundamental amplitude in my previous post: the amplitude of an electron to absorb or emit a photon. So let’s have a look at these three. As Feynman says: “āOut of these three amplitudes, **we can make theĀ **** whole world**, aside from what goes on in nuclei, and gravitation, as always!āĀ

Well… Thank you, Mr Feynman:Ā I’ve always wanted to understand the World (especially if *you* made it).

**The photon-electron coupling constant j**

Let’s start with the last of those three amplitudes (or wave functions): the amplitude of an electron to absorbĀ *orĀ *emit a photon. Indeed, absorbing or emitting makes no difference: we have the same complex number for both. It’s a constant – denoted by ** j**Ā (for

*j*unction

*Ā*number)Ā – equal to ā0.1 (a bit less actually but it’s good enough as an approximation

*in the context of this blog*).

*Huh?*Ā *Minus 0.1?Ā *That’s not a complex number, is it? It is. Real numbers are complex numbers too: ā0.1 is 0.1*e*^{iĻĀ }in polar coordinates. As Feynman puts it: it’s ** “a shrink to about one-tenth, and half a turn.”**Ā The ‘shrink’ is the 0.1 magnitude of this vector (or arrow), and the ‘half-turn’ is the angle of Ļ (i.e. 180 degrees). He obviously refers to

*multiplying (no adding here)*Ā

**with other amplitudes, e.g. P(A, C) and E(B, C) if the coupling is to happen at or near C. And, as you’ll remember, multiplying complex numbers amounts to adding their phases, and multiplying their modulus (so that’s adding the angles and multiplying lengths).**

*j*Let’s introduce a Feynman diagram at this point – drawn by Feynman himself – *which shows three possible ways of two electrons exchanging a photon*. We actually have two couplings here, and so the combined amplitude will involve two ** j**‘s. In fact, if we label the starting point of the two lines representing our electrons as 1 and 2 respectively, and their end points as 3 and 4, then the amplitude for these events will be given by:

E(1 to 5)Ā·** j**Ā·E(5 to 3)Ā·E(2 to 6)Ā·

**Ā·E(6 to 3)**

*j*Ā As for how thatĀ * jĀ *factor works,Ā please do read the caption of the illustration below: the same

*describes both emission as well as absorption. It’s just that we haveĀ*

**j**Ā*bothĀ*an emissionĀ

*as well as*Ā an as absorption here, so we have aĀ

**j**^{2 }factor here, which is less than 0.1Ā·0.1 = 0.01. At this point, it’s worth noting that it’s obvious that the amplitudes we’re talking about here – i.e. for

*one possible way*Ā of an exchange like the one below happening – are very tiny. They only become significant when we add

*many*of these amplitudes, which – as explained below – is what has to happen: one has to consider all possible paths, calculate the amplitudes for them (through multiplication), and then add all these amplitudes, to then – finally – square the modulus of the combined ‘arrow’ (or amplitude) to get

*some probability*of

*something actually happening*. [Again, that’s the best we can do: calculate probabilities that correspond to experimentally measured occurrences. We cannot

*predictĀ*anything in the classical sense of the word.]

A Feynman diagram is not just some sketchy drawing. For example, we have to care about scales: the distance and time units are equivalent (so distance would be measured in light-seconds or, else, time would be measured in units equivalent to the time needed for light to travel one meter). Hence, particles traveling through time (and space) – from the bottom of the graph to the top – will usuallyĀ *notĀ *Ā be traveling at an angle of more than 45 degrees (as measured from the time axis) but, from the graph above, it is clear that photons do. [Note that electrons moving through spacetime are represented by plain straight lines, while photons are represented by wavy lines. It’s just a matter of convention.]

More importantly,* a Feynman diagram is a pictorial device showing what needs to be calculated and how. *Indeed, with all the complexities involved, it is easy to lose track of what should be added and what should be multiplied, especially when it comes to much more complicated situations like the one described above (e.g. making sense of a scattering event). So, while the coupling constant ** j** (aka as the ‘charge’ of a particle – but it’s obviously not the electric charge) is just a number, calculating an actual E(A to B) amplitudes is not easy – not only because there are many different possible routes (paths) but because (almost) anything can happen. Let’s have a closer look at it.

**E(A to B)**

As Feynman explains in his 1985 QED *Lectures*: “E(A to B) can be represented as a giant sum of a lot of different ways an electron can go from point A to B in spacetime: the electron can take a ‘one-hop flight’, going directly from point A to B; it could take a ‘two-hop flight’, stopping at an intermediate point C; it could take a ‘three-hop flight’ stopping at points D and E, and so on.”

Fortunately, the calculation re-uses known values: the amplitude for each *‘hop’* – from C to D, for example – is P(F to G) – so that’s the amplitude of aĀ *photon *(!)Ā to go from F to G – even if we are talking an electron here. But there’s a difference: we *alsoĀ *have to multiply the amplitudes for each ‘hop’ with the amplitude for each *‘stop’*, and that’s represented by another number – not ** j** but

**. So we have an infinite series of terms for E(A to B): P(A to B) + P(A to C)Ā·**

*n*^{2}*n*

^{2}Ā·P(C to B)Ā + P(A to D)Ā·

*n*

^{2}Ā·P(D to E)Ā·

*n*

^{2}Ā·P(E to B) + …Ā

*for all possible intermediate points C, D, E, and so on*, as per the illustration below.

You’ll immediately ask: what’s the value of *n*? It’s quite important to know it, because we want to know how big these *n*^{2},Ā *n*^{4Ā }etcetera terms are. I’ll be honest: I have not come to terms with that yet. According to Feynman (QED, p. 125), it is the ‘rest mass’ of an ‘ideal’ electron: an ‘ideal’ electron is an electron that doesn’t know Feynman’s amplitude theory and just goes from point to point in spacetime *using only the direct path*. š Hence, it’s not a probability amplitude like ** j**: a properĀ probability amplitude will always have a modulus less than 1, and so when we see exponential terms like

*j*^{2},

*j*^{4},… we know we should not be all that worried – because these sort of vanish (go to zero) for sufficiently large exponents. For E(A to B), we do

*notĀ*have such vanishing terms. IĀ will not dwell on this rightĀ

*here*, but I promise to discuss it in the

*Post ScriptumĀ*of this post. The frightening possibility is that

*n*might beĀ a number

*larger*than one.

[As we’re freewheeling a bit anyway here, just a quick note on conventions: I should not be writingĀ *j**Ā *in bold-face, because it’s a (complex- or real-valued) *number* and symbols representing numbers are usually *notĀ *written in bold-face: *vectors* are written in bold-face. So, while you can look at a complex number as a vector, well… It’s just one of these inconsistencies I guess. The problem with using bold-face letters to represent complex numbers (like amplitudes) is that they suggest that the ‘dot’ in a product (e.g. *j*Ā·*j*) is an actual *dot projectĀ *(aka as a scalar product or an *innerĀ *product) of two vectors. That’s not the case. We’re multiplying complex numbers here, and so we’re just using the standard definition of a product of complex numbers. This subtlety probably explains why Feynman prefers to write the above product as P(A to B) + P(A to C)**n*^{2}*P(C to B)Ā + P(A to D)**n*^{2}*P(D to E)**n*^{2}*P(E to B) + … But then I find that using that asterisk to represent multiplication is a bit funny (although it’s a pretty common thing in complex math) and so *I* am *not* using it. Just be aware that a dot in a product may not always mean the same type of multiplication: multiplying complex numbers and multiplying vectors is *not *the same. […] And I won’t write ** j** in bold-face anymore.]

**P(A to B)**

Regardless of the value for *n*,Ā it’s obvious we need a functional form for *P(A to B)*, because that’s the other thing (other than *n*) that we need to calculate E(A to B). *So what’s the amplitude of a photon to go from point A to B*?

Well… The function describing P(A to B) is obviously some wave function – so that’s a complex-valued function of x and t. It’s referred to as a (Feynman) ** propagator**: a propagator functionĀ gives the probability amplitude for a particle to travel from one place to another in a given time, or to travel with a certain energy and momentum. [So our function for E(A to B) will be a propagator as well.] You can check out the details on it on Wikipedia. Indeed, IĀ

*couldĀ*insert the formula here, but believe me if I say it would only confuse you. The points to note is that:

- The propagator is also derived from the wave equation describing the system, so that’s some kind of differential equation which incorporates the relevant rules and constraints that apply to the system. For electrons, that’s the SchrĆ¶dinger equation I presented in my previous post. For photons… Well… As I mentioned in my previous post, there is ‘something similar’ for photons – there
*mustĀ*be –Ā but I have not seen anything that’s equally ‘simple’ as the SchrĆ¶dinger equation for photons. [I haveĀ*Googled*Ā a bit but it’s obvious we’re talking pretty advanced quantum mechanics here – so it’s not the QM-101 course that I am currently trying to make sense of.]*Ā* - The most important thing (in this context at least) is that the key variable in
*this*propagator (i.e. the Feynman propagator for the photon) is*I*: thatĀ**spacetime interval**which I mentioned in my previous post already:

*I* = Īr^{2Ā }ā Īt^{2}Ā = Ā (z_{2}– z_{1})^{2Ā }+Ā (y_{2}– y_{1})^{2Ā }+Ā (x_{2}– x_{1})^{2Ā }āĀ (t_{2}–Ā t_{1})^{2}

In this equation, we need to measure the time and spatial distance between two points in spacetime *in equivalent units*Ā (these ‘points’ are usually referred to as *four-vectors*), so weād use light-seconds for the unit of distance or, for the unit of time, the time it takes for light to travel one meter.Ā [If we don’t want to transform time or distance scales, then we have to writeĀ *I*Ā as *I =Ā **c*^{2}Īt^{2}Ā āĀ Īr^{2}.] Now, there are three types of intervals:

- For
**time-like intervals**, we have a*negative*Ā value for*I*, so Īt^{2Ā }> Īr^{2}. For two events separated by a time-like interval, enough time passes between them so there*could*be a causeāeffect relationship between the two events. In a Feynman diagram, the angle between the time axis and the line between the two events will be less than 45 degrees from the vertical axis. The traveling electrons in the Feynman diagrams above are an example. - For
**space-like intervals**, we have a*positive*value for*I*, so Īt^{2Ā }< Īr^{2}. Events separated by space-like intervals cannot possibly be causally connected. The photons traveling between point 5 and 6 in the first Feynman diagram are an example, but then*photonsĀ do have amplitudes to travel faster than light.* - Finally, for
**light-like intervals**,*I*= 0, orĀ Īt^{2 }= Īr^{2}. The points connected by the 45-degree lines in the illustration below (which Feynman uses to introduce his Feynman diagrams) are an example of points connected by light-like intervals.

[Note that we are using the so-called space-like convention (+++ā) here for *I*. There’s also a time-like convention, i.e. withĀ +āāā as signs: *I* =Ā Īt^{2}Ā āĀ Īr^{2Ā }so just check when you would consult other sources on this (which I recommend) and if you’d feel I am not getting the signs right.]

Now, what’s the relevance of this? To calculate P(A to B), we have toĀ *addĀ *the amplitudesĀ *for all possible pathsĀ *that the photon can take, and not in space, but *in spacetime*. So we should add all these *vectors* (or ‘arrows’ as Feynman calls them) – an infinite number of them really. In the meanwhile, you know it amounts to adding complex numbers, and that infinite sums are done by doing integrals, but let’s take a step back: how are vectors added?

Well…That’s easy, you’ll say… It’s the parallelogram rule… Well… Yes. And no. Let me take a step back here to show *how adding a whole range of similar amplitudes works*.

The illustration below shows a bunch of photons – real or imagined – from a source above a water surface (the sun for example), all taking *different paths* to arrive at a detector under the water (let’s say some fish looking at the sky from under the water). In this case, we make abstraction of all the photons *leaving at different timesĀ *and so we only look at a bunch that’s leaving at the same point in time. In other words, theirĀ stopwatches will be synchronized (i.e. there is no *phase shift *term*Ā *in the phase of their wave function) – let’s say at 12 o’clock when they leave the source. [If you think this simplification is not acceptable, well… Think again.]

When these stopwatches hit the *retina *of our poor fish’s eye (I feel we should put a detector there, instead of a fish), they will stop, and the hand of each stopwatch represents an amplitude: it has a modulus (its length) – which is assumed to be the same because all paths are equally likely (this is one of the first principles of QED) – *but their direction is very different*. However, by now we are quite familiar with these operations: we add all the ‘arrows’ indeed (or vectors or amplitudes or complex numbers or whatever you want to call them) and get one ** big** final arrow, shown at the bottom – just above the caption. Look at itĀ

*very carefully.*

If you look at the so-calledĀ *contribution* made by each of the individual arrows, you can see that it’s the arrows associated with the path of least time and the paths immediately left and right of it that make the biggest *contributionĀ *to the final arrow. Why? Because ** these stopwatches arrive around the same time and, hence, their hands point more or less in the same direction**. It doesn’t matter what direction – as long as it’s more or less

*the same*.

[As for the calculation of the path of least time, that has to do with the fact that light is slowed down in water. Feynman shows why in his 1985 *Lectures on QED*, but I cannot possibly copy the whole book here ! The principle is illustrated below.] Ā

So, where are we? This digressions go on and on, don’t they? Let’s go back to the main story: we want to calculate P(A to B), remember?

As mentioned above, one of the first principlesĀ in QED is that all paths – in spacetime – are equally likely. So we need to add amplitudes for every possible path in spacetime using that Feynman propagator function. You can imagine that will be some kind of integral which you’ll never want to solve. Fortunately, Feynman’s disciples have done that for you already. The results is quite predictable: **the grand result is that light has a tendency to travel in straight lines and at the speed of light.**

* WHAT!? *Did Feynman get a Nobel prize for trivial stuff like that?

Yes. The math involved in adding amplitudes over all possible paths not only in space but also in time uses the so-called path integral formulation of quantum mechanics and so that’s got Feynman’s signature on it, and that’s the main reason why he got this award – together with Julian Schwinger and Sin-Itiro Tomonaga: both much less well known than Feynman, but so they shared the burden. Don’t complain about it. Just take a look at the ‘mechanics’ of it.

We already mentioned that the propagator has the spacetime interval *I*Ā in its denominator. Now, the way it works is that, for values of *I*Ā *equal or close to zero*, so the paths that are associated with light-like intervals, our propagator function will yield *large* contributions in the ‘same’ direction (wherever that direction is), but for the spacetime intervals that are very much time- or space-like, the magnitude of our amplitude will be smaller and – worse – our arrow will point in the ‘wrong’ direction. In short, the arrows associated with the time- and space-like intervals don’t add up to much, especially over longer distances. [When distances are short, there are (relatively) few arrows to add, and so the probability distribution will be flatter: in short, the likelihood of having the *actual*Ā photon travel faster or slower than speed is higher.]

**Conclusion**

Does this make sense? I am not sure, but I did what I promised to do. I told you how *P(A to B)* gets calculated; and from the formula for E(A to B), it is obvious that we can then also calculate *E(A to B)*Ā **provided we have a value for n**. However, that value

*n*is determined experimentally, just like the value of

*j*, in order to ensure this amplitude theory yields probabilities that match the probabilities we observe in all kinds of crazy experiments that try to prove or disprove the theory; and then we can use these three amplitude formulas “to make the whole world”, as Feynman calls it, except the stuff that goes on

*inside of nucleiĀ*(because that’s the domain of the weak and strong nuclear force) and gravitation, for which we have aĀ

*law*(Newton’s Law)Ā but no real ‘explanation’. [Now, you may wonder if this QED explanation of light is really all that good, but Mr Feynman thinks it is, and so I have no reason to doubt that – especially because there’s surely not anything more convincing lying around as far as I know.]

So what remains to be told? Lots of things, even *within* the realm of expertise of quantum electrodynamics. Indeed, Feynman applies the basics as described above to a number ofĀ *real-lifeĀ *phenomena – quite interesting, all of it ! – but, once again, it’s not my goal to copy all of his *LecturesĀ *here. [I am only hoping to offer some good summaries of key points in some attempt to convince myself that I am getting some of it at least.] And then there is the strong force, and the weak force, and the Higgs field, and so and so on. But that’s all very strange and new territory which I haven’t even started to explore. I’ll keep you posted as I am making my way towards it.

**Post scriptum**: On the values of *j* and *n*

In this post, I promised I would write something about how we can find *j* and *n*Ā because I realize it would just amount to copy three of four pages out of that book I mentioned above, and which inspired most of this post. Let me just say something more about that remarkable book, and then quote a few lines on what the author of that book – the great Mr Feynman ! – thinks of the math behind calculating these two constants (the coupling constantĀ *j*, and the ‘rest mass’Ā of an ‘ideal’ electron). Now, before I do that, I should repeat that he actually *invented* that math (it makes use of a mathematical approximation method called perturbation theory) and that *he gotĀ **a Nobel Prize for it.*

First, about the book. Feynman’s 1985 *Lectures on Quantum ElectrodynamicsĀ *are not like his 1965* Lectures on Physics.Ā *The *Lectures on PhysicsĀ *are proper courses for undergraduate and even graduate students in physics. This little 1985 book on QED is justĀ a series of four lectures for a lay audience, conceived in honor of *Alix G. Mautner*. She was a friend of Mr Feynman’s who died a few years before he gave and wrote these ‘lectures’ on QED. She had a degree in English literature and would ask Mr Feynman regularly to explain quantum mechanics and quantum electrodynamics in a way she would understand. While they had known each other for about 22 years, he had apparently never taken enough time to do so, as he writes in his Introduction to these *Alix G. Mautner MemorialĀ Lectures*: *“So here are the lectures I really [should have] prepared for Alix, but unfortunately I can’t tell them to her directly, now.”*

The great Richard Phillips Feynman himself died only three years later, in February 1988 – not of one but *twoĀ *rare forms ofĀ cancer. He was only 69 years old when he died. I don’t know if he was aware of the cancer(s) that would kill him, but I find his fourth and last lecture in the book, *Loose Ends*, just **fascinating**. Here we have aĀ *brilliant mind*Ā deprecating the math that earned him a Nobel Prize and *without which the Standard Model would be unintelligible*. I won’t try to paraphrase him. Let me just quote him. [If you want to check the quotes, the relevant pages are page 125 to 131):

The math behind calculating these constants] is **a ādippy processā** and ā** having to resort to such hocus-pocus has prevented us from proving that the theory of quantum electrodynamics is mathematically self-consistent**ā. He adds: ā

**Itās surprising that the theory still hasnāt been proved self-consistent one way or the other by now; I suspect that**renormalization [“

**the shell game that we play to find n and j**” as he calls it]

**Ā is not mathematically legitimate.**ā […] Now,Ā Mr Feynman writes this about quantum electrodynamics, not aboutĀ

*āthe rest of physicsā*Ā (and so thatās quantum chromodynamics (QCD) ā the theory of the strong interactions ā and quantum flavordynamics (QFD) ā the theory of weak interactions) which, he adds,Ā

*āhas not been checked anywhere near as well as electrodynamics.āĀ*

Thatās a pretty damning statement, isnāt it? In one of my other posts (see:Ā *The End of the Road to Reality?*), I explore these comments a bit. However, I have to admit I feel I really need to get back to math in order to appreciate these remarks. I’ve written way too much about physics anyway now (as opposed to the my first dozen of posts – which were much more math-oriented). So I’ll just have a look at some more stuff indeed (such as perturbation theory), and then I’ll get back blogging.Ā Indeed, I’ve written like 20 posts or so in a few months only – so I guess I should shut up for while now !

In the meanwhile, you’re more than welcome to comment of course !Ā