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4 - String Diagrams

Published online by Cambridge University Press:  30 March 2017

Bob Coecke
Affiliation:
University of Oxford
Aleks Kissinger
Affiliation:
Radboud Universiteit Nijmegen
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Summary

When two systems, of which we know the states by their respective representatives, enter into temporary physical interaction due to known forces between them, and when after a time of mutual influence the systems separate again, then they can no longer be described in the same way as before, viz. by endowing each of them with a representative of its own. I would not call that one but rather the characteristic trait of quantum mechanics, the one that enforces its entire departure from classical lines of thought.

Erwin Schrödinger, 1935

By 1935, Schrödinger had already realised that the biggest gulf between quantum theory and our received classical preconceptions is that, when it comes to quantum systems, the whole is more than the sum of its parts. In classical physics, for instance, it is possible to totally describe the state of two systems – say, two objects sitting on a table – by first totally describing the state of the first system then totally describing the state of the second system. This is a fundamental property one expects of a classical, separable universe. However, as Schrödinger points out, there exist states predicted by quantum theory (and observed in the lab!) that do not obey this ‘obvious’ law about the physical world. Schrödinger called this new, totally non-classical phenomenon Verschränkung, which later became translated to the dominant scientific language as entanglement.

Quantum picturalism is all about studying the way parts compose to form a whole. In the good company of Schrödinger, we believe that the role of multiple interacting systems – especially non-separable systems – should take centre stage in the study of quantum theory.

We shall see in the next section that it is easy to say what it means for a process to be separable in terms of diagrams. Literally, it means that it can be broken up into pieces that are not connected to each other. On the other hand, enforcing non-separability requires us to refine our diagrammatic language. To this end, we introduce special states and effects called cups and caps, respectively. Intuitively, cups and caps act like pieces of wire that have been ‘bent sideways’.

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Picturing Quantum Processes
A First Course in Quantum Theory and Diagrammatic Reasoning
, pp. 83 - 153
Publisher: Cambridge University Press
Print publication year: 2017

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  • String Diagrams
  • Bob Coecke, University of Oxford, Aleks Kissinger, Radboud Universiteit Nijmegen
  • Book: Picturing Quantum Processes
  • Online publication: 30 March 2017
  • Chapter DOI: https://doi.org/10.1017/9781316219317.005
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  • String Diagrams
  • Bob Coecke, University of Oxford, Aleks Kissinger, Radboud Universiteit Nijmegen
  • Book: Picturing Quantum Processes
  • Online publication: 30 March 2017
  • Chapter DOI: https://doi.org/10.1017/9781316219317.005
Available formats
×

Save book to Google Drive

To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Google Drive.

  • String Diagrams
  • Bob Coecke, University of Oxford, Aleks Kissinger, Radboud Universiteit Nijmegen
  • Book: Picturing Quantum Processes
  • Online publication: 30 March 2017
  • Chapter DOI: https://doi.org/10.1017/9781316219317.005
Available formats
×