Creation and annihilation operators

Results: 23



#Item
1Probabilities versus Amplitudes John Baez, Jacob Biamonte, Brendan Fong Mathematical Trends in Reaction Network Theory 1 July 2015

Probabilities versus Amplitudes John Baez, Jacob Biamonte, Brendan Fong Mathematical Trends in Reaction Network Theory 1 July 2015

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Source URL: math.ucr.edu

Language: English - Date: 2015-07-01 06:01:09
2HW #11 (221B), due Apr 22, 4pm 1. Suppose annihilation and creation operators satisfy the standard commutation relation [a, a† ] = 1. (a) Show that the Bogliubov transformation b = a cosh η + a† sinh η (1)

HW #11 (221B), due Apr 22, 4pm 1. Suppose annihilation and creation operators satisfy the standard commutation relation [a, a† ] = 1. (a) Show that the Bogliubov transformation b = a cosh η + a† sinh η (1)

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Source URL: hitoshi.berkeley.edu

Language: English - Date: 2014-01-31 18:26:59
    31 Ph 12b Homework Assignment No. 6 Due: 5pm, Thursday, 25 FebruaryGeometric phase (15 points).

    1 Ph 12b Homework Assignment No. 6 Due: 5pm, Thursday, 25 FebruaryGeometric phase (15 points).

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    Source URL: www.theory.caltech.edu

    Language: English - Date: 2010-02-19 16:40:58
    4Physics 521 University of New Mexico I. H. Deutsch Special Lecture Notes: Coherent States of a Simple Harmonic Oscillator The Simple Harmonic Oscillator

    Physics 521 University of New Mexico I. H. Deutsch Special Lecture Notes: Coherent States of a Simple Harmonic Oscillator The Simple Harmonic Oscillator

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    Source URL: info.phys.unm.edu

    Language: English - Date: 2002-10-10 17:23:19
    5Comparison of Dynamic Diffusion with an Explicit Difference Scheme for the Schrödinger Equation

    Comparison of Dynamic Diffusion with an Explicit Difference Scheme for the Schrödinger Equation

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    Source URL: www.complex-systems.com

    Language: English - Date: 2014-03-11 12:49:15
    6Spans and the Categorified Heisenberg Algebra – 1 John Baez for more, see: http://math.ucr.edu/home/baez/spans/

    Spans and the Categorified Heisenberg Algebra – 1 John Baez for more, see: http://math.ucr.edu/home/baez/spans/

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    Source URL: math.ucr.edu

    Language: English - Date: 2013-09-14 04:02:14
    7Ph125c lecture notes, Many-body systems; Bosons and Fermions The topic of many-body systems and particle statistics properly belongs to quantum field theory, but it is traditional to attempt to treat these subje

    Ph125c lecture notes, Many-body systems; Bosons and Fermions The topic of many-body systems and particle statistics properly belongs to quantum field theory, but it is traditional to attempt to treat these subje

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    Source URL: www.its.caltech.edu

    Language: English - Date: 2001-04-19 12:51:09
    8Week 6 (due Nov. 13) Reading: Srednicki, sections 6 and[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q 0 , q; T ) = hq 0 |e−iHT |qi. Here H is the usual Hamiltonian, i.e.

    Week 6 (due Nov. 13) Reading: Srednicki, sections 6 and[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q 0 , q; T ) = hq 0 |e−iHT |qi. Here H is the usual Hamiltonian, i.e.

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    Source URL: www.theory.caltech.edu

    Language: English - Date: 2009-11-07 12:59:11
    9Week 5 (due Nov. 7) Reading: Srednicki, sections 6 and[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q ′ , q; T ) = hq ′ |e−iHT |qi. Here H is the usual Hamiltonian, i.e.

    Week 5 (due Nov. 7) Reading: Srednicki, sections 6 and[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q ′ , q; T ) = hq ′ |e−iHT |qi. Here H is the usual Hamiltonian, i.e.

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    Source URL: www.theory.caltech.edu

    Language: English - Date: 2007-11-02 00:50:25
    10Week 4 (due Oct[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q 0 , q; T ) = hq 0 |e−iHT |qi. Here H is the usual Hamiltonian, i.e. H=

    Week 4 (due Oct[removed]The transition amplitude in nonrelativistic Quantum Mechanics is defined by K(q 0 , q; T ) = hq 0 |e−iHT |qi. Here H is the usual Hamiltonian, i.e. H=

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    Source URL: www.theory.caltech.edu

    Language: English - Date: 2013-10-24 00:38:18