(b) QuantizationThe Born interpretation puts severe restrictions on th terjemahan - (b) QuantizationThe Born interpretation puts severe restrictions on th Bahasa Indonesia Bagaimana mengatakan

(b) QuantizationThe Born interpreta

(b) Quantization

The Born interpretation puts severe restrictions on the acceptability of wavefunctions.
The principal constraint is that ψ must not be infinite anywhere.
If it were, the integral in eqn 7.20 would be infinite (in other words, ψ would not be square-integrable) and the normalization constant would be zero.
The normalized function would then be zero everywhere, except where it is infinite, which would be unacceptable.
The requirement that ψ is finite everywhere rules out many possible solutions of the Schrödinger equation, because many mathematically acceptable solutions rise to infinity and are therefore physically unacceptable.
We shall meet several examples shortly.
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(b) QuantizationThe Born interpretation puts severe restrictions on the acceptability of wavefunctions.The principal constraint is that ψ must not be infinite anywhere. If it were, the integral in eqn 7.20 would be infinite (in other words, ψ would not be square-integrable) and the normalization constant would be zero. The normalized function would then be zero everywhere, except where it is infinite, which would be unacceptable. The requirement that ψ is finite everywhere rules out many possible solutions of the Schrödinger equation, because many mathematically acceptable solutions rise to infinity and are therefore physically unacceptable. We shall meet several examples shortly.
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Hasil (Bahasa Indonesia) 2:[Salinan]
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(b) Quantization Interpretasi Born menempatkan pembatasan pada penerimaan fungsi gelombang. Kendala utama adalah bahwa ψ tidak harus dalam fi nite di mana saja. Kalau, integral di eqn 7.20 akan berhingga (dengan kata lain, ψ tidak akan persegi -integrable) dan konstanta normalisasi akan menjadi nol. Fungsi normal maka akan menjadi nol di mana-mana, kecuali itu adalah berhingga, yang akan diterima. Persyaratan bahwa ψ adalah fi nite di mana-mana aturan keluar banyak kemungkinan solusi dari persamaan Schrödinger, karena banyak matematis solusi yang dapat diterima naik ke dalam fi nity dan karena itu tidak dapat diterima secara fisik. Kita akan bertemu beberapa contoh lama.







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