# Difference between revisions of "Heisenberg Uncertainty Principle"

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A similar example is [[time]] and [[energy]], the product of which also has a lower limit. Quantum fluctuations are a result of this, where for short time, there is enough energy in "empty space" to create a pair of particle and antiparticle, such as [[electron]] and [[positron]]. Although this appears to be a strange or extreme process, it is the only one to explain some properties of black holes. Laser physics with ultrashort [[laser]] pulses is another field, where the limit in the product of time and energy plays an important role. | A similar example is [[time]] and [[energy]], the product of which also has a lower limit. Quantum fluctuations are a result of this, where for short time, there is enough energy in "empty space" to create a pair of particle and antiparticle, such as [[electron]] and [[positron]]. Although this appears to be a strange or extreme process, it is the only one to explain some properties of black holes. Laser physics with ultrashort [[laser]] pulses is another field, where the limit in the product of time and energy plays an important role. | ||

+ | |||

+ | ==Derivation== | ||

+ | |||

+ | It can be shown that for two operators, <math>\hat{A}</math> and <math>\hat{B}</math>, that do not [[Commutative|commute]] that there exists and uncertainty principle: | ||

+ | |||

+ | <math> | ||

+ | \sigma^2_a \sigma^2_b = \frac{1}{4} (\langle {\hat{A} \hat{B}} \rangle - \langle {\hat{B} \hat{A}} \rangle)^2 | ||

+ | </math> | ||

+ | |||

+ | For position and momentum, the relevant operators are <math>\hat{x} = x</math> and <math>\hat{p} = \frac{\hbar}{i} \frac{\partial}{\partial x}</math>, and it can be shown that <math>[\hat{x}, \hat{p}] = i \hbar</math>. This leads to the result above. | ||

+ | |||

[[Category:Quantum Mechanics]] | [[Category:Quantum Mechanics]] | ||

[[Category:Chemistry]] | [[Category:Chemistry]] |

## Revision as of 16:13, 22 November 2016

The **Heisenberg Uncertainty Principle** states that for any two quantum observables which do not commute, the product of the standard deviations of the measurements of those observables must be greater than or equal to a positive constant, related to Planck's constant ().

The most common example is of a particle's momentum and its position . Mathematically it is represented with this equation:

.

This means that we can never measure both the position and momentum of a particle simultaneously with arbitrary precision. The more precisely we wish to measure one observable, the less precisely we can measure the other at that time.

Contrary to popular belief, this is *not* merely a measurement issue. While it is often stated that it is not possible to know the precise position and momentum of a particle at the same time, this is misleading; this statement implies that the particle has precisely defined position and momentum, but that information is unavailable to us. In fact, the Uncertainty Principle tells us that a particle cannot have precisely defined position or momentum.

A similar example is time and energy, the product of which also has a lower limit. Quantum fluctuations are a result of this, where for short time, there is enough energy in "empty space" to create a pair of particle and antiparticle, such as electron and positron. Although this appears to be a strange or extreme process, it is the only one to explain some properties of black holes. Laser physics with ultrashort laser pulses is another field, where the limit in the product of time and energy plays an important role.

## Derivation

It can be shown that for two operators, and , that do not commute that there exists and uncertainty principle:

For position and momentum, the relevant operators are and , and it can be shown that . This leads to the result above.