Quantum information science

D-Wave Two

D-Wave Two (project code name Vesuvius) is the second commercially available quantum computer, and the successor to the first commercially available quantum computer, D-Wave One. Both computers were developed by Canadian company D-Wave Systems. The computers are not general purpose, but rather are designed for quantum annealing. Specifically, the computers are designed to use quantum annealing to solve a single type of problem known as quadratic unconstrained binary optimization. As of 2015, it was still debated whether large-scale entanglement takes place in D-Wave Two, and whether current or future generations of D-Wave computers will have any advantage over classical computers. (Wikipedia).

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Inside the D-Wave Quantum Computer

An animation showing the different systems inside D-Wave's quantum computers. Video made by: Dominic Walliman https://twitter.com/DominicWalliman Learn more about D-Wave and the first commercial quantum computers at https://www.dwavesys.com/

From playlist Videos I made for D-Wave Systems

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Waves and Particles B3 Compton Effect and De Broglie Wavelength

The Compton effect and De Broglie wavelength.

From playlist Physics - Wave Particle Duality

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Sending a Problem to the D-Wave Quantum Computer

Animation showing the process when a user submits a problem to the D-Wave quantum computer. Video made by: Dominic Walliman https://twitter.com/DominicWalliman Learn more about D-Wave and the first commercial quantum computers at https://www.dwavesys.com/

From playlist Videos I made for D-Wave Systems

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Waves 6_2 Doppler Effect

Solution to problems dealing with the Doppler effect.

From playlist Physics - Waves

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Waves 6_3 Doppler Effect

Solution to problems dealing with the Doppler effect.

From playlist Physics - Waves

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Waves 2_15 Superposition of Waves and Interference

The interference of identical waves

From playlist Physics - Waves

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Waves 6_1 Doppler Effect

Explaining the Doppler effect. Worked problems.

From playlist Physics - Waves

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D-Wave Lab Tour: The D-Wave Processor (Part 2)

In this video we look at the quantum annealing processor. We look at how it differs from regular processors, and how qubits encode 0s and 1s. Want to find out more? Check out our website https://www.dwavesys.com/ This is the third video of three that describe different aspects of the D-W

From playlist Videos I made for D-Wave Systems

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Waves II 1_2 Traveling Electromagnetic Waves

The electromagnetic wave from the Maxwell equations.

From playlist Physics - Waves

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Double & Single Slit Experiments and Diffraction Gratings

Describes the maths of the double and single slit experiments and the operation of the diffraction grating.

From playlist Quantum Mechanics

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Waves - A Level Physics

Continuing the A Level revision series with Waves. Looking at transverse and longitudinal waves, the electromagnetic spectrum, polarisation, interference, the single slit and double slit experiments, a diffraction grating, refraction and refractive indices.

From playlist A Level Physics Revision

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AS Physics Exam Questions: Waves

Examples of exam questions at Physics AS level for Waves covering Edexcel, AQA and OCR material.

From playlist A Level Physics Exam Questions - Worked Examples

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Mod-01 Lec-13 Debye Theory of Specific Heat, Lattice Vibrations

Condensed Matter Physics by Prof. G. Rangarajan, Department of Physics, IIT Madras. For more details on NPTEL visit http://nptel.iitm.ac.in

From playlist NPTEL: Condensed Matter Physics - CosmoLearning.com Physics Course

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What is light?

Demonstrating that light is electromagnetic radiation from Maxwell's equations and how it is propagated.

From playlist Electricity & Magnetism

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4. Solutions to Schrödinger Equation, Energy Quantization

MIT 2.57 Nano-to-Micro Transport Processes, Spring 2012 View the complete course: http://ocw.mit.edu/2-57S12 Instructor: Gang Chen License: Creative Commons BY-NC-SA More information at http://ocw.mit.edu/terms More courses at http://ocw.mit.edu

From playlist MIT 2.57 Nano-to-Micro Transport Processes, Spring 2012

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Lectures 2 & 3 | Quantum Entanglements, Part 3 (Stanford)

Lectures 2 and 3 of Leonard Susskind's course concentrating on Quantum Entanglements (Part 3, Spring 2007). Recorded April 2007 at Stanford University. This Stanford Continuing Studies course is the third of a three-quarter sequence of classes exploring the "quantum entanglements" in mo

From playlist Lecture Collection | Quantum Entanglements: Part 3 (Spring 2007)

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Lecture 14: Resonance and the S-Matrix

MIT 8.04 Quantum Physics I, Spring 2013 View the complete course: http://ocw.mit.edu/8-04S13 Instructor: Allan Adams In this lecture, Prof. Adams discusses the resonance structure of a potential barrier/well. He begins with the case of simple plane waves and then moves on to the case of w

From playlist MIT 8.04 Quantum Physics I, Spring 2013 (2013)

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الاهتزازات والأمواج (جامعة إم آي تي) - المحاضرة 13: الأمواج الكهرومغناطيسيَّة، الاستقطاب

MIT المحاضرة الثالثة عشرة من مساق "الاهتزازات والأمواج" من جامعة إم آي تي للبروفيسور والتر لوين وهي عن الأمواج الكهرومغناطيسيَّة، الاستقطاب بالإضافة للفيديو هناك ملفات مرفقة على موقعنا الالكتروني https://shamsunalarabia.net/courses/الاهتزازات-والأمواج/ رابط المساق https://www.youtube.com/

From playlist 8.03 Arabic Subtitles

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Waves II 1_1 Traveling Electromagnetic Waves

Introduction to electromagnetic waves.

From playlist Physics - Waves

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Jérémie Szeftel The resolution of the bounded L2 curvature conjecture in General Relativity (Part 1)

In order to control locally a space-­time which satisfies the Einstein equations, what are the minimal assumptions one should make on its curvature tensor? The bounded L2 curvature conjecture roughly asserts that one should only need L2 bounds of the curvature tensor on a given space-like

From playlist Ecole d'été 2014 - Analyse asymptotique en relativité générale

Related pages

Qubit | Quantum entanglement | CPLEX | Simulated annealing | Quadratic unconstrained binary optimization | Quantum annealing | D-Wave Systems