Attempts to theoretically explain the observed emission spectrum of the Hydrogen atom were initiated as soon as the spectrum was observed starting with Ångström in 1853, followed by Balmer 1885 who discovered an algebraic formula 3 years later generalised by Rydberg into
- $\frac{1}{\lambda}=R_H (\frac{1}{n_1^2}-\frac{1}{n_2^2})$ (R)
where $\lambda$ is wave length, $R_H$ is Rydberg's constant, and $1\le n_1<n_2$ are natural numbers.
The challenge was to find a mathematical model of the H atom which reproduced (R). Bohr in the 1910s came up with an ad hoc model in terms of classical mechanics, but the real breakthrough came in 1926 when the 38 year old Austrian physicist Erwin Schrödinger formulated an eigenvalue problem for a partial differential equation which he could solve analytically and so find to exactly agree with (R). This model was coined Schrödinger's Equation SE and was formulated in terms of a wave function $\Psi (x)$ with $\Psi^2(x)$ representing electronic charge density and $x$ a spatial Euclidean 3d coordinate. The success was complete and rocketed Schrödinger to fame.
At the same time the young 24 year old Werner Heisenberg from a different school of physics had developed another mathematical model as a new form of algebraic model named matrix mechanics with focus on what could be measured (the spectrum) rather than on underlying physics like Schrödinger. It turned out that the two models could be identified. But it was Schrödinger who insisted on a physically meaningful model, not only formality fitted to observation.
Anyway, Heisenberg supported by his mentor Max Born took over the scene by developing a SE for systems with many electrons by a purely formal mathematical generalisation by adding a new 3d coordinate for each new electron.
So was the foundation of modern physics as Standard Quantum Mechanics StdQM as a Schrödinger Equation SE in terms of a (complex-valued) wave function $\Psi (x)$ depending on a spatial coordinate $x$ which ranges over a configuration space with $3N$ dimensions (plus a time coordinate $t$), by Born given the following meaning to be named the Copenhagen Interpretation CI:
- $\vert\Psi (x)\vert^2$ is a probability density of configurations $x\in\Re^{3N}$.
But a probability density does not represent any actuality of physical nature, only a possibility of physical nature. Since reality consists of actualities and not of possibilities, many physicists including Schrödinger and Einstein, did not find CI convincing. Later other interpretations were tried to give the wave function over configuration space physical meaning (Bohm, Many Worlds,...), but on the whole were less convincing.
The result is that modern physics still today is based on a mathematical model in the form of SE in wave function over configuration space, for which the physical meaning is lacking. This means that the message to students of modern physics from the highest authorities of theoretical physics including many Nobel Laureates today is something like:
- Do not worry/ask about physical meaning of solutions to SE. There is no answer.
- Accept that predictions about physics from solving SE always agree with experimental observation.
Of course this is not a healthy situation and the result is a crisis of modern physics deepening with each Nobel Prize to StdQM.
In any case, textbooks present StdQM and then in particular teaches about superposition as basic element of atom physics not present in classical physics, and recall Schrödinger's Cat which can both alive and dead at the same time, as a wave function $\Psi =\Psi_a + \Psi_d$ with $\Psi_a$ representing a live cat and $\Psi_d$ a dead with the + sign still to give a physical meaning.
The student will be told that the spectrum of an atom arises from superpositions of eigenstates with different eigenvalues which allows the superposition to express a beat frequency as a difference of eigenvalues. But the physics of the beat frequency will be unclear because the physics of the eigenstates are.
The physical origin of an emission line in the spectrum must be a physical dipole generated by oscillating electron charge densities, but the connection to beat frequency in superposition lacks physics because eigenstates lack physics.
RealQM is an alternative to StdQM based on non-overlapping electron densities with direct physical presence which directly connects to a dipole origin of the spectrum. In short, RealQM is a reformulation of StdQM into a model with direct physical interpretation as non-overlapping charge densities. The clear physicality in the case $N=1$ is kept when going to $N>1$.
The basic problem with StdQM is lack of physics for $N>1$. RealQM comes with physics for $N>1$.
A restart from SE with $N=1$ appears to be necessary, and RealQM delivers an option.
Comment by chatGPT:
Your post makes a passionate case for re-examining the foundations of quantum mechanics, particularly the move from Schrödinger’s single-electron wave equation to the high-dimensional configuration-space formalism used in standard quantum mechanics (StdQM). It’s true that the interpretation of the wave function — whether it *represents physical reality or only a probability distribution — has been debated since the early days of the theory, and this debate continues in the physics community. csc.kth.se+1
However, it’s important to separate formal mathematical success from interpretational issues. Standard quantum mechanics predicts experimental outcomes with extremely high precision across countless systems, from atomic spectra to quantum field theory and particle physics. Its use of a wave function on configuration space and probabilistic interpretation (as in the Born rule) may seem abstract, but these features are not just philosophical; they match observation. math.columbia.edu
Interpretational discomfort — like Schrödinger’s own unease with the Copenhagen Interpretation or Einstein’s critiques — doesn’t mean the theory is wrong. Many physicists acknowledge that interpretations (Copenhagen, Many-Worlds, Bohmian mechanics, etc.) differ yet agree on observable predictions. math.columbia.edu
If your RealQM approach can reproduce all known experimental results and make new, testable predictions, then the physics community would certainly be interested. The real challenge for any alternative formulation is not just providing a more intuitive picture, but showing it agrees with all precise experimental data where standard quantum mechanics excels.