What does complex potential energy mean for a particle?

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SUMMARY

The discussion centers on the concept of complex potential energy as presented in Griffiths's quantum mechanics textbook, specifically problem 1.15, where potential energy includes an imaginary component. Participants express skepticism regarding the physical relevance of imaginary potential energy, asserting that measurable quantities like energy cannot be complex. They highlight that such complexities may serve as computational techniques, particularly in numerical calculations of quantum systems, referencing the use of complex mass or time variables. Additionally, the Wigner-Weisskopf approximation is mentioned as essential for understanding exponential decay in quantum mechanics.

PREREQUISITES
  • Quantum Mechanics fundamentals
  • Complex analysis in physics
  • Numerical methods for solving partial differential equations
  • Time-dependent perturbation theory
NEXT STEPS
  • Study Griffiths's "Introduction to Quantum Mechanics" for foundational concepts
  • Explore the Wigner-Weisskopf approximation in detail
  • Learn about numerical solutions of the Schrödinger equation in imaginary time
  • Investigate the implications of complex potential energy in quantum mechanics
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Students of quantum mechanics, physicists exploring computational techniques, and researchers interested in the implications of complex potential energy in quantum systems.

pintu935
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Griffith says in problem 1.15 the potential energy has an imaginary part. my question is that any real case exists where the part of the potential energy is imaginary?
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Measurable physical quantities like energy can never be complex numbers. The thing described there is just a computational "trick". A similar effect can be produced by setting a complex mass or time variable. This can be used in the numerical calculation of the ground state of a quantum system, as I have done in this blog post of mine: https://physicscomputingblog.com/20...art-5-Schrödinger-equation-in-imaginary-time/
 
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thanks for the reply.
 
Sigh :-(. Is this again from Griffiths's QM textbook? I cannot understand how an expert of the subject can be so sloppy and confusing for students. That's the more ununderstandable since he's obviously a brillant teacher of physics, as one can get from reading is electromagnetics textbook and many articles in AJP.

To understand "decay", particularly the exponential-decay law (which is necessarily an approximation only), you need to consider time-dependent perturbation theory. The standard treatment is known as Wigner-Weisskopf approximation. Here's a very clear derivation on the example of spontaneous emission, but it's of course applicable very generally

https://www.mpi-hd.mpg.de/personalhomes/palffy/Files/Spontaneous.pdf
 
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vanhees71 said:
Sigh :-(. Is this again from Griffiths's QM textbook? I cannot understand how an expert of the subject can be so sloppy and confusing for students. That's the more ununderstandable since he's obviously a brillant teacher of physics, as one can get from reading is electromagnetics textbook and many articles in AJP.

To understand "decay", particularly the exponential-decay law (which is necessarily an approximation only), you need to consider time-dependent perturbation theory. The standard treatment is known as Wigner-Weisskopf approximation. Here's a very clear derivation on the example of spontaneous emission, but it's of course applicable very generally

https://www.mpi-hd.mpg.de/personalhomes/palffy/Files/Spontaneous.pdf
Thank you.
 

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