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北星論集(短) 第 13 号(通巻第51号) March 2015

量子力学的状態の周期的軌道としての解釈

内 山   智

Satoshi UCHIYAMA

目次 1.はじめに 2.周期的軌道を量子力学的状 態とする模型 3.確率の打ち消し合いに関す る考察 [Abstract]

An Interpretation of Quantum-mechanical States As Periodic Trajectories

 A hidden variable model is proposed under such an interpretation that a quantum-mechanical state corresponds to a periodic trajectory in a classical phase space. In this model, a parameter that is the angle variable of the periodic trajectory corresponds to the phase factor of the corresponding wave function. During the measurement process of each physical quantity, the physical system is influenced by its environment, including the measuring apparatus, and the prepared periodic trajectory is deformed. In this model, this deformation is approximated by representing it as a result of a bifurcation of the trajectory. Even though the trajectory is deformed, if the information corresponding to the phase factor is not lost, then the deformed trajectory is interpreted as the same quantum-mechanical state. A mechanism of interference of probability amplitudes is also considered.

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量子力学的状態の周期的軌道としての解釈

偶関数とするならば、

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─ 86 ─

يಓΛ χ

γ

(nβ1,··· ,nN)

i

))

ͱදΘ͢ͱ͠Α͏ɻ

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(n′1,··· ,n′N) γ

i

)

ͱͷؔ܎͸Ͳ͏ͳΔ

͔ؾʹͳΔɻn

k

΍ n

′k

͕େ͖͘ͳͬͨͱͯ͠

΋ɺχ

γ

(nβ1,··· ,nN)

i

))

ͱ χ

(n′ 1,··· ,n′N) γ

i

)

͸

౳͘͠͸͋Δ·͍ɻ͜ΕΒ͕ಉ͡౷ܭతੑ࣭

Λ࣋ͭͱ͍͏ྔࢠྗֶత֬཰Λ࠶ݱ͢ΔͨΊ

ʹ͸ɺP (θ) = | cos θ| ͱஔ͘ඞཁ͕͋Δɻͦ

͏͢Δ͜ͱͰɺώϧϕϧτۭؒͷϰΣΫτϧ

ͱରԠ෇͚͕ՄೳʹͳΔ͔ΒͰ͋Δ [3]ɻ͢Δ

ͱɺγ = α ͱஔ͍ͨͱ͖ɺj ̸= i ʹ͍ͭͯɺ

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j

= α

j

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χ

(n′1,··· ,n′N) α

i

) = α

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ɺ͋Δ͍͸ l(α

i

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ʹର͢Δଌఆ݁Ռ͕

੔߹తʹͳΔɻ

[

ࢀߟจݙ

]

[1]

಺ࢁɹஐ, “ྔࢠྗֶతঢ়ଶʹ͍ͭͯ”, ๺

੕ֶԂେֶ୹ظେֶ෦๺੕࿦ू, 10, 59–

65 (2013).

[2] S. Uchiyama, “Local Reality: Can It

Exist in the EPR–Bohm Gedanken

Ex-periment?”, Found. Phys. , 25 (1995)

1561–1575.

[3]

಺ࢁɹஐ, “ྔࢠॏͶ߹ΘͤݪཧͷҰͭͷ

ղऍʹ͍ͭͯ”, ๺੕ֶԂେֶ୹ظେֶ෦

๺੕࿦ू, 8, 1–7 (2010).

[4]

಺ࢁɹஐ, “ۉߧݪཧͱྔࢠྗֶత֬཰

”,

๺੕ֶԂେֶ୹ظେֶ෦๺੕࿦ू, 9,

33–41 (2011).

[5]

಺ࢁɹஐ, “ۉߧݪཧʹجͮ͘ྔࢠྗֶ

తաఔʹΑΔෳ߹ܥͷऔΓѻ͍”, ๺੕

ֶԂେֶ୹ظେֶ෦๺੕࿦ू, 10, 13–21

(2012).

[6]

಺ࢁɹஐ, “ྔࢠྗֶతաఔͷଌఆ݁Ռͷ

ඇہॴੑʹ͍ͭͯ”, ๺੕ֶԂେֶ୹ظେ

ֶ෦๺੕࿦ू, 11, 67–70 (2013).

6

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