REVIEW
Supersymmetry and Quantum Mechanics
High Energy Physics - Theory · Submitted 4 May 1994 · 265 references
Pith's verdict: The standard SUSY QM reference, and it holds up; the one soft spot that lands is the series-defined scaling potentials in Sec. 4.3.2, not the classification claim the reader flagged.
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Referee report
The paper
The paper claims
The review argues that shape invariance is the common algebraic reason a large family of quantum potentials is exactly solvable.
The reading
What carries the argument
Shape invariance is the load-bearing mechanism: the two SUSY partner potentials $V_1=W^2-W'$ and $V_2=W^2+W'$ are required to have the same spatial form after a parameter transformation, $V_2(x;a_1)=V_1(x;a_2)+R(a_1)$. That condition turns the Riccati/factorization structure into a ladder: $H_s$ has ground energy $�sum_{k=1}^{s-1}R(a_k)$, so the original spectrum is the partial sums of $R$, while $A^�dagger(x;a_k)$ maps one rung to the next. The same condition is what makes the SWKB quantization condition exact in the translation case and what organizes the new scaling and multi-step potentials.
Extended reading notes
Core claim
The central claim is that shape invariance, $V_2(x;a_1)=V_1(x;a_2)+R(a_1)$, is the organizing integrability condition behind the standard analytically solvable potentials. Starting from a factorized Hamiltonian $H_1=A^�dagger A$ with superpotential $W(x)$, the SUSY partner is $H_2=AA^�dagger$; when the partner potentials differ only by a parameter map and an $x$-independent remainder, the whole bound-state spectrum follows as $E_n=�sum_{k=1}^n R(a_k)$ with $E_0=0$, and the eigenfunctions follow from repeated application of $A^�dagger$. The review presents the translation case $a_2=a_1+�alpha$ as covering the familiar textbook potentials, adds scaling and multi-step variants, and argues that the lowest-order SWKB quantization condition is exact for the translation-type shape-invariant class. It also uses the same machinery to generate isospectral potentials and multi-soliton KdV solutions and to exhibit supersymmetry in Pauli and Dirac problems.
Load-bearing premise
The load-bearing premise is that the translation-type shape-invariance classification built from the factorized superpotential ansatz in Eq. (130) captures the standard analytically solvable potentials, even though the authors state they have no rigorous proof that the ansatz exhausts the class.
Editorial extensions
If this is right
- For any potential whose SUSY partner is shape invariant with a translation parameter map, the bound-state energies can be written down as partial sums of the remainder without solving a differential equation.
- The eigenfunctions of the same class are generated algebraically from the ground state by repeated application of the operators $A^�dagger(x;a_k)$.
- The lowest-order supersymmetric WKB quantization condition reproduces the exact spectrum for translation-type shape-invariant potentials, unlike ordinary WKB.
- The scaling and multi-step shape-invariance constructions produce new reflectionless potentials with infinite bound-state spectra, including q-deformed relatives of the Rosen-Morse and oscillator potentials.
- The same SUSY bookkeeping yields n-parameter isospectral families and explicit multi-soliton solutions of the KdV hierarchy.
Reading between the lines
- If shape invariance is the right organizing principle, it gives a practical test for exact solvability: compute the SUSY partner and check whether it closes under a parameter map before attempting a direct integration.
- A useful next test would be to look for a closed-form expression for one of the series-defined scaling superpotentials; success would turn that class from a formal construction into a directly usable potential family.
- The isospectral families can be read as a control knob: one can change a potential's shape and scattering data while holding its bound-state energies fixed, which is a natural setting for testing whether tunneling rates depend on barrier shape beyond the energy splitting.
- Singular superpotentials, which the review uses to produce negative-energy states and bound states in the continuum, suggest that the same SUSY bookkeeping could classify which singular potentials admit normalizable states embedded in the continuum.
Original abstract
In the past ten years, the ideas of supersymmetry have been profitably applied to many nonrelativistic quantum mechanical problems. In particular, there is now a much deeper understanding of why certain potentials are analytically solvable and an array of powerful new approximation methods for handling potentials which are not exactly solvable. In this report, we review the theoretical formulation of supersymmetric quantum mechanics and discuss many applications. Exactly solvable potentials can be understood in terms of a few basic ideas which include supersymmetric partner potentials, shape invariance and operator transformations. Familiar solvable potentials all have the property of shape invariance. We describe new exactly solvable shape invariant potentials which include the recently discovered self-similar potentials as a special case. The connection between inverse scattering, isospectral potentials and supersymmetric quantum mechanics is discussed and multi-soliton solutions of the KdV equation are constructed. Approximation methods are also discussed within the framework of supersymmetric quantum mechanics and in particular it is shown that a supersymmetry inspired WKB approximation is exact for a class of shape invariant potentials. Supersymmetry ideas give particularly nice results for the tunneling rate in a double well potential and for improving large $N$ expansions. We also discuss the problem of a charged Dirac particle in an external magnetic field and other potentials in terms of supersymmetric quantum mechanics. Finally, we discuss structures more general than supersymmetric quantum mechanics such as parasupersymmetric quantum mechanics in which there is a symmetry between a boson and a para-fermion of order $p$.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
In the past ten years, the ideas of supersymmetry have been profitably applied to many nonrelativistic quantum mechanical problems. In particular, there is now a much deeper understanding of why certain potentials are analytically solvable and an array of powerful new approximation methods for handling potentials which are not exactly solvable. In this report, we review the theoretical formulation of supersymmetric quantum mechanics and discuss many applications. Exactly solvable potentials can be understood in terms of a few basic ideas which include supersymmetric partner potentials, shape invariance and operator transformations. Familiar solvable potentials all have the property of shape invariance. We describe new exactly solvable shape invariant potentials which include the recently discovered self-similar potentials as a special case. The connection between inverse scattering, isospectral potentials and supersymmetric quantum mechanics is discussed and multi-soliton solutions of the KdV equation are constructed. Approximation methods are also discussed within the framework of supersymmetric quantum mechanics and in particular it is shown that a supersymmetry inspired WKB approximation is exact for a class of shape invariant potentials. Supersymmetry ideas give particularly nice results for the tunneling rate in a double well potential and for improving large $N$ expansions. We also discuss the problem of a charged Dirac particle in an external magnetic field and other potentials in terms of supersymmetric quantum mechanics. Finally, we discuss structures more general than supersymmetric quantum mechanics such as parasupersymmetric quantum mechanics in which there is a symmetry between a boson and a para-fermion of order $p$.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | In the past ten years, the ideas of supersymmetry have been profitably applied to many nonrelativistic quantum mechanical problems. | background 1.00 | 0.05 | 0.07 | asserted 1.00 |
| s1 | In particular, there is now a much deeper understanding of why certain potentials are analytically solvable and an array of powerful new approximation methods for handling potentials which are not exactly solvable. | background 0.99 | 0.07 | 0.11 | asserted 1.00 |
| s2 | In this report, we review the theoretical formulation of supersymmetric quantum mechanics and discuss many applications. | contribution 0.98 | 0.50 | 0.11 | asserted 0.75 |
| s3 | Exactly solvable potentials can be understood in terms of a few basic ideas which include supersymmetric partner potentials, shape invariance and operator transformations. | background 0.40 | 0.20 | 0.12 | asserted 1.00 |
| s4 | Familiar solvable potentials all have the property of shape invariance. | background 0.64 | 0.13 | 0.06 | asserted 1.00 |
| s5 | We describe new exactly solvable shape invariant potentials which include the recently discovered self-similar potentials as a special case. | contribution 0.93 | 0.91 | 0.11 | asserted 1.00 |
| s6 | The connection between inverse scattering, isospectral potentials and supersymmetric quantum mechanics is discussed and multi-soliton solutions of the KdV equation are constructed. | contribution 0.82 | 0.76 | 0.06 | asserted 0.98 |
| s7 | Approximation methods are also discussed within the framework of supersymmetric quantum mechanics and in particular it is shown that a supersymmetry inspired WKB approximation is exact for a class of shape invariant potentials. | result 0.72 | 0.84 | 0.12 | asserted 1.00 |
| s8 | Supersymmetry ideas give particularly nice results for the tunneling rate in a double well potential and for improving large $N$ expansions. | result 0.84 | 0.58 | 0.07 | asserted 0.96 |
| s9 | We also discuss the problem of a charged Dirac particle in an external magnetic field and other potentials in terms of supersymmetric quantum mechanics. | contribution 0.98 | 0.59 | 0.03 | asserted 0.92 |
| s10 | Finally, we discuss structures more general than supersymmetric quantum mechanics such as parasupersymmetric quantum mechanics in which there is a symmetry between a boson and a para-fermion of order $p$. | contribution 0.92 | 0.57 | 0.07 | asserted 0.91 |
What was examined, and what was not
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Figures
Showing 4 of the paper's 12 figures. See all figures in the PDF ↗ Figures reproduced from arXiv:hep-th/9405029 by the authors.
References
How later papers used it
220 later papers cite it
4 later papers by other authors are listed below: 4 used its method or tool.
Uses its method or tool 4 of 27 papers with this label
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Obtained exact solutions for spin waves in the backgrounds of static and precessing domain walls with the aid of supersymmetric quantum mechanics from this paper.
Propulsion of a domain wall in an antiferromagnet by magnons (2014) · 0.99 · paraphrased: the licence does not allow quoting
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Interestingly, the usual test for the essential self-adjointness of a symmetric operator is greatly simplified by the fact that the symmetric operator can be understood as a hamiltonian of supersymmetric quantum mechanics (SQM) [ref] .
Supersymmetric Backgrounds in $(1+1)$ Dimensions and Inhomogeneous Field Theory (2022) · Introduction · 0.86
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After obtaining the ground state energy ($E_0$) and wave function ($ψ_0(r)$), a one-parameter family of IP [equation] can be constructed following Nieto 1984 [ref] , Khare and Sukhatme 1989 [ref] , and Cooper et al. 1995 [ref] applying formalism of SSQM.
Resonance energy and wave functions of $^{31}$Ne: a calculation using supersymmetric quantum mechanics (2022) · Construction of one-parameter family of IP using SSQM · 0.99
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Rewrote its equation as a zero-eigenvalue mode Schrödinger equation and understood it in the context of supersymmetric quantum mechanics from this paper, identifying a superpotential.
Inflating baby-Skyrme branes in six dimensions (2010) · 0.80 · paraphrased: the licence does not allow quoting
How the literature uses it
162 arXiv papers cite this in 259 sentences
Papers citing it · 144 sentences without a confident label
Builds on it 1 paper
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The fermionic operators [equation] generate an $sl(1|1)$ superalgebra [ref] , [equation] where [equation] and $S_3$ is defined by [equation] Choosing $H$ as the Hamiltonian, we get a system that generalizes the usual $N=2$ supersymmetry of a spin-$1/2$ particle with gyromagnetic ratio $g=2$ in arbitrary magnetic field [ref] to the non-commutative case.
Super-extended noncommutative Landau problem and conformal symmetry · $N=2$ supersymmetry: arbitrary magnetic field · 0.90
Uses its method or tool 14 papers
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They are obtained by Darboux–Crum transformations [ref] applied to the exactly solvable Schrödinger equations [ref] of the radial oscillator potential and the Pöschl–Teller potential.
Global Solutions of Certain Second-Order Differential Equations with a High Degree of Apparent Singularity · Introduction · 0.94
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Eq.([ref]) can be rewritten in the form of a zero-eigenvalue mode Schrödinger equation for the function [equation] namely [equation] where the potential is [equation] Eq.([ref]) can be understood in the context of so called the supersymmetric quantum mechanics [ref] where the function $W(r)$ is identified as the superpotential in the SUSY QM.
Inflating baby-Skyrme branes in six dimensions · Stability of the Baby-skyrmions with fixed gravitational background · 0.80
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Interestingly, the usual test for the essential self-adjointness of a symmetric operator is greatly simplified by the fact that the symmetric operator can be understood as a hamiltonian of supersymmetric quantum mechanics (SQM) [ref] .
Supersymmetric Backgrounds in $(1+1)$ Dimensions and Inhomogeneous Field Theory · Introduction · 0.86
Compares with it 4 papers
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Potentials: [equation] [equation] where $V_0$ is an irrelevant constant given by [equation] Solvable sectors: [equation] It is worth mentioning here that the potential $V^(0)+(q)$ coincides with the potential whose bound state wave functions are given in terms of exceptional $X_1$ Jacobi polynomial [ref] for $a=1$, $b_1=B+/2$, $z_0=-(2A-1)/(2B)$ whereas potential $V^(0)-(q)$ coincides with the Scarf I potential [ref] [after making an change $B→B+$] whose bound state wave functions are given in terms of classical Jacobi polynomials.
Effect of Position-dependent Mass on Dynamical Breaking of Type B and Type X_2 N-fold Supersymmetry · Effects of PDM on Dynamical Symmetry Breaking of Type B $$-fold SUSY · 0.97
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Such a representation reveals an obvious similarity of the hidden supersymmetry of the spinless Aharonov-Bohm system with supersymmetry of a usual form, associated with introduction of the spin degrees of freedom [ref] .
Hidden superconformal symmetry of spinless Aharonov-Bohm system · Hidden N=2 supersymmetry in spinless AB system · 0.88
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Note relative simplicity of the found potential in a comparison with variety of the reflectionless shape invariant potentials (with scaling of parameters; for example, see [ref] ).
Double complex SUSY-transformations: deformations of real potentials and their spectral characteristics · Conclusions · 1.00
Cites it as background 78 papers
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Their exact solvability is due to the fact that they satisfy the property of shape invariance [ref] , which was initially developed in one-dimensional supersymmetric quantum mechanics with real potential [ref] and was later on generalized to higher-dimensional systems [ref] .
Ladder Operators and Hidden Algebras for Shape Invariant Nonseparable and Nondiagonalizable Modelswith Quadratic Complex Interaction. I. Two-Dimensional Model · Introduction · 0.81
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In this section, after recapitulating the radial oscillator [ref] and the Laguerre polynomial [ref] , we present its free oscillator realization.
Free Oscillator Realization of the Laguerre Polynomial · Radial Oscillator and Free Oscillator Realization · 0.97
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For such a purpose, we have used an approach inspired by a branch of supersymmetric quantum mechanics [ref] , whose development dates back to that of quantum groups and $q$-algebras [ref] .
Point Canonical Transformation versus Deformed Shape Invariance for Position-Dependent Mass Schr\"odinger Equations · Introduction · 0.81
Discussion
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