Entropy: Difference between revisions

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Updated to include Renyi entropy functionality
m Fix latex-isms
 
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: <math>S_\alpha(\rho) := \frac{1}{1-\alpha}\log_2\big(\mathrm{Tr}(\rho^\alpha)\big)</math>
: <math>S_\alpha(\rho) := \frac{1}{1-\alpha}\log_2\big(\mathrm{Tr}(\rho^\alpha)\big)</math>


(i.e., the Rényi-$\alpha$ entropy).
(i.e., the Rényi-<math>\alpha</math> entropy).


==Syntax==
==Syntax==
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</syntaxhighlight>
</syntaxhighlight>


A d-by-d maximally-mixed state has entropy $\log_2(d)$:
A d-by-d maximally-mixed state has entropy <math>\log_2(d)</math>:
<syntaxhighlight>
<syntaxhighlight>
>> Entropy(eye(4)/4)
>> Entropy(eye(4)/4)
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==Notes==
==Notes==
The Rényi-$\alpha$ entropy approaches the von Neumann entropy as $\alpha \rightarrow 1$.
The Rényi-<math>\alpha</math> entropy approaches the von Neumann entropy as <math>\alpha \rightarrow 1</math>.


{{SourceCode|name=Entropy}}
{{SourceCode|name=Entropy}}

Latest revision as of 16:59, 4 August 2023

Entropy
Computes the von Neumann or Rényi entropy of a density matrix

Other toolboxes required none
Function category Information theory

Entropy is a function that computes the von Neumann entropy or Rényi entropy of a density matrix. That is, given a density matrix $\rho$, it computes the following quantity:

<math>S(\rho) := -\mathrm{Tr}\big(\rho\log_2(\rho)\big)</math>

(i.e., the von Neumann entropy) or the following quantity:

<math>S_\alpha(\rho) := \frac{1}{1-\alpha}\log_2\big(\mathrm{Tr}(\rho^\alpha)\big)</math>

(i.e., the Rényi-<math>\alpha</math> entropy).

Syntax

  • ENT = Entropy(RHO)
  • ENT = Entropy(RHO,BASE)
  • ENT = Entropy(RHO,BASE,ALPHA)

Argument descriptions

  • RHO: A density matrix to have its entropy computed.
  • BASE (optional, default 2): The base of the logarithm used in the entropy calculation.
  • ALPHA (optional, default 1): A non-negative real parameter that determines which entropy is computed (ALPHA = 1 corresponds to the von Neumann entropy, otherwise the Rényi-ALPHA entropy is computed).

Examples

The extreme cases: pure states and maximally-mixed states

A pure state has entropy zero:

>> Entropy(RandomDensityMatrix(4,0,1)) % entropy of a random 4-by-4 rank-1 density matrix

ans =

   7.3396e-15 % silly numerical errors: this is effectively zero

A d-by-d maximally-mixed state has entropy <math>\log_2(d)</math>:

>> Entropy(eye(4)/4)

ans =

     2

All other states have entropy somewhere between these two extremes:

>> Entropy(RandomDensityMatrix(4))

ans =

    1.6157

Notes

The Rényi-<math>\alpha</math> entropy approaches the von Neumann entropy as <math>\alpha \rightarrow 1</math>.

Source code

Click here to view this function's source code on github.