The misterious 'inverted' harmonic oscillator

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SUMMARY

The discussion centers on the 'inverted' harmonic oscillator defined by the Hamiltonian H=p² - ωx². This system lacks bound states due to a saddle point at (0,0), leading to non-periodic classical solutions represented by Asinh(ωt) + Bcosh(ωt). In quantum mechanics, the wave functions do not belong to L²(-∞, ∞), resulting in a continuous spectrum with no discrete eigenvalues. Consequently, a particle in this potential continuously gains momentum as x approaches ±∞, illustrating that it does not function as a traditional oscillator.

PREREQUISITES
  • Understanding of Hamiltonian mechanics
  • Familiarity with classical and quantum oscillators
  • Knowledge of continuous spectra in quantum mechanics
  • Basic concepts of L² spaces in functional analysis
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  • Research the implications of saddle points in Hamiltonian systems
  • Explore the mathematical properties of non-periodic solutions in classical mechanics
  • Study the concept of continuous spectra in quantum mechanics
  • Investigate applications of inverted harmonic oscillators in theoretical physics
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The discussion is beneficial for theoretical physicists, quantum mechanics students, and researchers exploring advanced concepts in Hamiltonian dynamics and spectral theory.

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given the Hamiltonian [tex]H=p^{2}- \omega x^{2}[/tex]

we can see inmediatly that this Hamiltonian will NOT have a BOUND state due to a 'saddle point' on (0,0) , here 'omega' is the frecuency of the Harmonic oscillations

the classical solutions are not PERIODIC [tex]Asinh( \omega t) +Bcosh( \omega t)[/tex]

The Quantum counterpart is even worse since the functions will NOT be on [tex]L^{2} (-\infty , \infty )[/tex] then how is the spectrum ?

is there any webpage where this oscillator is considered ? What applications can be found ??
 
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There is no spectrum, the eigenvalues are continuous. A particle in this potential would gain momentum continuously as x goes to plus or minus infinity.

Like a ball on a hill.

It is not an oscillator.
 

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