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www3.eng.cam.ac.uk/~sh372/index.xml
www3.eng.cam.ac.uk/~sh372/index.xml15 Jan 2024: 2021-fan-cnf-droplet/ Wed, 24 Feb 2021 00:00:00 0000 http://www.eng.cam.ac.uk/sh372/publication/2021-fan-cnf-droplet/ Compositional and entropy indirect noise generated in ... measuring fine-to-ultrafine aerosols using bipolar charge equilibrium -
Simone Hochgreb –
www3.eng.cam.ac.uk/~sh372/files/cv.pdf15 Jan 2024: 2022 How fast can we burn, 2.0, Keynote, 39th Symposium on Combustion, July 24-30,Vancouver, Canada. -
Theoretical Physics II
www.tcm.phy.cam.ac.uk/~rjs269/TP2/TP2y2024.pdf22 Jan 2024: 1.23)The evolution operator is. U(t) =. U1(t) 0 t < t1U2(t t1)U1(t1) t1 t < t2 (1.24)where Ui(t) = eiHi t/h̄ and Hi =. p22m. ... This is Feynman’spath integral. 24. 2.2 The propagator. The path integral is a tool for calculating the propagator -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/UKMMNTalk2023.pdf3 Apr 2023: Slide 22. Slide 23. Slide 24. Slide 25. Slide 26. Slide 27. -
Slide 1
www.tcm.phy.cam.ac.uk/~gjc29/talks/PhysicsByTheLakeTalk2023.pdf22 Aug 2023: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/IndiaTalk2023.pdf24 Jul 2023: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/EMMCTalk2023.pdf28 Apr 2023: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CICECOTalk2023.pdf27 Jun 2023: Slide 20. Slide 21. Slide 22. Slide 23. Slide 24. Slide 25. -
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www.tcm.phy.cam.ac.uk/~gjc29/talks/CICECODoctoralTalk2023.pdf29 Sep 2023: Slide 24. Slide 25. Slide 26. Slide 27. Slide 28. Slide 29. -
Unveil the unseen: Exploit information hidden in noise
www.tcm.phy.cam.ac.uk/~gjc29/papers/ZviazhynskiConduit22.pdf23 May 2023: Furthermore, the uncertainty is useful foraccelerating materials discovery by guiding where newexperiments should be performed in the materials space[22–24], and also for the identification of outliers anderroneous entries in
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