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n the mathematically rigorous formulation of quantum mechanics, the state of a quantum mechanical system is a vector {\displaystyle \psi }\psi belonging to a (separable) complex Hilbert space {\displaystyle {\mathcal {H}}}{\mathcal {H}}. This vector is p

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量子力学の数学的に厳密な定式化では、量子力学系の状態は、(分離可能な) 複素ヒルベルト空間に属するベクトル {\displaystyle \psi }\psi です {\displaystyle {\mathcal {H}}}{\mathcal {H}}。このベクトルは p です

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In a mathematically rigorous formulation of quantum mechanics, the states of a quantum mechanical system are vectors {\displaystyle \psi }\psi belonging to a (separable) complex Hilbert space {\displaystyle {\mathcal {H}}} {\mathcal {H}}. This vector is p

INTO JAPANESE

量子力学の数学的に厳密な定式化では、量子力学系の状態は、(分離可能な) 複素ヒルベルト空間に属するベクトル {\displaystyle \psi }\psi {\displaystyle {\mathcal {H}}} {\mathcal { H}}。このベクトルは p です

BACK INTO ENGLISH

In a mathematically rigorous formulation of quantum mechanics, the states of a quantum mechanical system are the vectors {\displaystyle \psi }\psi {\displaystyle {\mathcal {H}}} that belong to the (separable) complex Hilbert space \mathcal { H}}. This vector is p

INTO JAPANESE

量子力学の数学的に厳密な定式化では、量子力学系の状態は、(分離可能な) 複素ヒルベルト空間 \mathcal に属するベクトル {\displaystyle \psi }\psi {\displaystyle {\mathcal {H}}} です。 {H}}。このベクトルは p です

BACK INTO ENGLISH

In a mathematically rigorous formulation of quantum mechanics, the states of a quantum mechanical system are the vectors {\displaystyle \psi }\psi {\displaystyle {\mathcal {H}} } is. {H}}. This vector is p

INTO JAPANESE

量子力学の数学的に厳密な定式化では、量子力学系の状態はベクトル {\displaystyle \psi }\psi {\displaystyle {\mathcal {H}} } です。 {H}}。このベクトルは p です

BACK INTO ENGLISH

In the mathematically rigorous formulation of quantum mechanics, the state of a quantum mechanical system is the vector {\displaystyle \psi }\psi {\displaystyle {\mathcal {H}} } . {H}}. This vector is p

INTO JAPANESE

量子力学の数学的に厳密な定式化では、量子力学系の状態はベクトル {\displaystyle \psi }\psi {\displaystyle {\mathcal {H}} } です。 {H}}。このベクトルは p です

BACK INTO ENGLISH

In the mathematically rigorous formulation of quantum mechanics, the state of a quantum mechanical system is the vector {\displaystyle \psi }\psi {\displaystyle {\mathcal {H}} } . {H}}. This vector is p

Equilibrium found!

That didn't even make that much sense in English.

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