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1 - 10 of 13 search results for katalk:PC53 24 / |u:www.qi.damtp.cam.ac.uk where 0 match all words and 13 match some words.

  1. Results that match 1 of 2 words

  2. Undergraduate and Masters (Part III) Lecture Courses | Centre for…

    www.qi.damtp.cam.ac.uk/undergraduate-and-masters-part-iii-lecture-courses
    8 May 2024: We offer the following Masters courses in 2023-24:. Prof Adrian Kent - Quantum Information, Foundations and Gravity (M16, examinable). ... Dr Berry Groisman - Topics in Quantum Foundations (16 lectures). Prof Nilanjana Datta - Quantum Information Theory

  3. Publications | Centre for Quantum Information and Foundations

    www.qi.damtp.cam.ac.uk/publications?page=11
    8 May 2024: A Kent. – Risk Anal. (2004). 24,. 157. (doi: 10.1111/j.0272-4332.2004.00419.x). Illustrating the concept of quantum information.

  4. Part III Quantum Computation | Centre for Quantum Information and…

    www.qi.damtp.cam.ac.uk/part-iii-quantum-computation
    8 May 2024: Quantum Computation. Lecturer: Sergii Strelchuk. Lent Term (24 lectures). Course times: t.b.c.

  5. Part IIC Lent term 2021 QUANTUM INFORMATION AND COMPUTATION ...

    www.qi.damtp.cam.ac.uk/files/PartIIIQC/Part%20IIC%20QIC/PartIIC%20QIClectures%20Full.pdf
    27 Sep 2021: Part IIC Lent term 2021. QUANTUM INFORMATION. AND COMPUTATION. Lecture notesRichard Jozsa, DAMTP Cambridge. rj310@cam.ac.uk. CONTENTS1 Introduction: why quantum computation and information? 32 Principles of quantum mechanics and the Dirac bra-ket

  6. Part IIC (January 2019 version) Lent term 2019 QUANTUM ...

    www.qi.damtp.cam.ac.uk/files/PartIIIQC/Part%202%20QIC%20lecturenotes.pdf
    4 Sep 2019: Part IIC (January 2019 version) Lent term 2019. QUANTUM INFORMATION. AND COMPUTATION. Lecture notesRichard Jozsa, DAMTP Cambridge. rj310@cam.ac.uk. CONTENTS1 Introduction: why quantum computation and information? 32 Principles of quantum mechanics

  7. 7 The 3D Schrödinger equation 7.1 Quantum mechanics in ...

    www.qi.damtp.cam.ac.uk/files/Adrian/notespart5.2019.pdf
    20 Nov 2019: 2M(d2ψ. dr2+. 2. r. dψ. dr) e. 2. 4π0rψ(r) = Eψ(r) , (7.24). ... polynomials.24. The corresponding wavefunctions are ψ(r) = CL1N1(2br) exp(br), where theconstant C is determined by normalisation.

  8. 6 The basic formalism of quantum mechanics 6.1 Spaces ...

    www.qi.damtp.cam.ac.uk/files/Adrian/notespart4.completed.2019.pdf
    1 Dec 2019: ψ, ABψ)|2 = 14(|(ψ, {A, B}ψ)|2 |(ψ, [A, B]ψ)|2). (6.26). Combining (6.24) and (6.26), we have that. ( ... Hence. (x̂ x̂ψ)ψ = ia(p̂ p̂ψ)ψ ,. which means we have equality in the Schwarz’s inequality (6.24) used to derive(6.28).

  9. 5 Tunnelling and Scattering Let us reconsider the bound ...

    www.qi.damtp.cam.ac.uk/files/Adrian/notespart3.completed.2019.pdf
    12 Nov 2019: FI =km. (5.24). FR =km. |R|2 = km. (k lk l.

  10. 4 Solutions of the 1D Schrödinger equation We now ...

    www.qi.damtp.cam.ac.uk/files/Adrian/notespart2.completed.2019.pdf
    6 Nov 2019: 4.24). 36. Hence. either A = 0 , sin(ka) = 0 ,. ψ(x) = B sin(kx) , k =nπ. 2afor n 2 even.

  11. Part IB Quantum Mechanics, Michaelmas 2019 Tuesday and Thursday, ...

    www.qi.damtp.cam.ac.uk/files/Adrian/notes311219.pdf
    3 Jan 2020: those satisfying Eqn. (3.11). 24. 3.3 The 1D Schrödinger equation for a particle in a potential.

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