I Understanding the Irreducible Solution in Classical Harmonic Oscillators

George444fg
Messages
25
Reaction score
4
TL;DR Summary
Harmonic Oscillator
Hellow. I am doing an introductory to Quantum Mechanics course, and the irreducible solution appeared in the harmonic oscillator. When we talk about the irreducible solution, this is the solution as a linear combination of the eigenbasis of the system. This is understandable, however, if I have a simple case of a harmonic oscillator, with solution sin(wt) then the irreducible solution would be ie^(-iwt)? Thank you in advance
 
Physics news on Phys.org
I'm a little confused by the terminology you use, particularly irreducible solution. But I read your post as defining the irreducible solution as the solution written as the sum of eigenvectors. Also, are you referring to the quantum harmonic oscillator or the classical harmonic oscillator in the last half of your post?
 
Haborix said:
I'm a little confused by the terminology you use, particularly irreducible solution. But I read your post as defining the irreducible solution as the solution written as the sum of eigenvectors. Also, are you referring to the quantum harmonic oscillator or the classical harmonic oscillator in the last half of your post?
It is the classic oscillator. But nonetheless, it can be derived from the quantum oscillator.
 
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles. Towards the end of the first lecture for the Qiskit Global Summer School 2025, Foundations of Quantum Mechanics, Olivia Lanes (Global Lead, Content and Education IBM) stated... Source: https://www.physicsforums.com/insights/quantum-entanglement-is-a-kinematic-fact-not-a-dynamical-effect/ by @RUTA
I am reading WHAT IS A QUANTUM FIELD THEORY?" A First Introduction for Mathematicians. The author states (2.4 Finite versus Continuous Models) that the use of continuity causes the infinities in QFT: 'Mathematicians are trained to think of physical space as R3. But our continuous model of physical space as R3 is of course an idealization, both at the scale of the very large and at the scale of the very small. This idealization has proved to be very powerful, but in the case of Quantum...
Thread 'Lesser Green's function'
The lesser Green's function is defined as: $$G^{<}(t,t')=i\langle C_{\nu}^{\dagger}(t')C_{\nu}(t)\rangle=i\bra{n}C_{\nu}^{\dagger}(t')C_{\nu}(t)\ket{n}$$ where ##\ket{n}## is the many particle ground state. $$G^{<}(t,t')=i\bra{n}e^{iHt'}C_{\nu}^{\dagger}(0)e^{-iHt'}e^{iHt}C_{\nu}(0)e^{-iHt}\ket{n}$$ First consider the case t <t' Define, $$\ket{\alpha}=e^{-iH(t'-t)}C_{\nu}(0)e^{-iHt}\ket{n}$$ $$\ket{\beta}=C_{\nu}(0)e^{-iHt'}\ket{n}$$ $$G^{<}(t,t')=i\bra{\beta}\ket{\alpha}$$ ##\ket{\alpha}##...
Back
Top