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A '''qutrit''' is a unit of [[quantum information]] that can exist in three possible states.
 
The qutrit is analogous to the classical [[Ternary numeral system|trit]], just as the [[qubit]], a quantum particle of two possible states, is analogous to the classical [[bit]].
 
==Representation==
A qutrit has three orthogonal [[Basis (linear algebra)|basis]] states, or [[vector space|vector]]s, often denoted <math>|0\rangle</math>, <math>|1\rangle</math>, and <math>|2\rangle</math> in Dirac or [[bra-ket notation]].
These are used to describe the qutrit as a [[Superposition principle|superposition]] in the form of a linear combination of the three states:
:<math>|\psi\rangle = \alpha |0\rangle + \beta |1\rangle + \gamma |2\rangle</math>,
where the coefficients are [[probability amplitude]]s, such that the sum of their squares is unity:
: <math>| \alpha |^2 + | \beta |^2 + | \gamma |^2 = 1 \,</math>
 
The qutrit's basis states are orthogonal. Qubits achieve this by utilizing [[Hilbert space]] <math>H_2</math>, corresponding to spin-up and spin-down. Qutrits require a Hilbert space of higher dimension, namely <math>H_3</math>.
 
A string of ''n'' qutrits represents 3<sup>''n''</sup> different states simultaneously.
 
Qutrits have several peculiar features when used for storing quantum information. For example, they are more robust to [[decoherence]] under certain environmental interactions.<ref>A. Melikidze, V. V. Dobrovitski, H. A. De Raedt, M. I. Katsnelson, and B. N. Harmon, ''Parity effects in spin decoherence'', Phys. Rev. B '''70''', 014435 (2004) ([http://link.aps.org/doi/10.1103/PhysRevB.70.014435 link])</ref> In reality, manipulating qutrits directly might be tricky, and one way to do that is by using an [[quantum entanglement|entanglement]] with a [[qubit]].<ref>B. P. Lanyon,1 T. J. Weinhold, N. K. Langford, J. L. O'Brien, K. J. Resch, A. Gilchrist, and A. G. White''Manipulating Biphotonic Qutrits'', Phys. Rev. Lett. '''100''', 060504 (2008) ([http://link.aps.org/abstract/PRL/v100/e060504 link])</ref>
 
==See also==
*[[Mutually unbiased bases]]
*[[Quantum computing]]
 
==References==
{{reflist}}
 
==External links==
*[http://www.physorg.com/news123244300.html Physicists Demonstrate Qubit-Qutrit Entanglement] by Lisa Zyga at [[Physorg.com]], February 26, 2008 . Accessed March 2008
 
{{quantum computing}}
 
[[Category:Units of information]]
[[Category:Quantum information science]]

Revision as of 09:32, 28 February 2013

A qutrit is a unit of quantum information that can exist in three possible states.

The qutrit is analogous to the classical trit, just as the qubit, a quantum particle of two possible states, is analogous to the classical bit.

Representation

A qutrit has three orthogonal basis states, or vectors, often denoted |0, |1, and |2 in Dirac or bra-ket notation. These are used to describe the qutrit as a superposition in the form of a linear combination of the three states:

|ψ=α|0+β|1+γ|2,

where the coefficients are probability amplitudes, such that the sum of their squares is unity:

|α|2+|β|2+|γ|2=1

The qutrit's basis states are orthogonal. Qubits achieve this by utilizing Hilbert space H2, corresponding to spin-up and spin-down. Qutrits require a Hilbert space of higher dimension, namely H3.

A string of n qutrits represents 3n different states simultaneously.

Qutrits have several peculiar features when used for storing quantum information. For example, they are more robust to decoherence under certain environmental interactions.[1] In reality, manipulating qutrits directly might be tricky, and one way to do that is by using an entanglement with a qubit.[2]

See also

References

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External links

Template:Quantum computing

  1. A. Melikidze, V. V. Dobrovitski, H. A. De Raedt, M. I. Katsnelson, and B. N. Harmon, Parity effects in spin decoherence, Phys. Rev. B 70, 014435 (2004) (link)
  2. B. P. Lanyon,1 T. J. Weinhold, N. K. Langford, J. L. O'Brien, K. J. Resch, A. Gilchrist, and A. G. White, Manipulating Biphotonic Qutrits, Phys. Rev. Lett. 100, 060504 (2008) (link)