Правка разделов «Statement», «Solution», «Answer»

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@@ -1,11 +1,5 @@
### Statement
−$14.5.24.$ [Insert the problem statement]
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−### Solution
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−### Statement
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$14.5.24.$ Prove that a free electron can neither absorb nor emit a photon.
### Solution
@@ -25,7 +19,7 @@Solution
$$(mc^2)^2 + 2mc^2 h\nu + (h\nu)^2 = (h\nu)^2 + m^2 c^4$$
After canceling out identical terms, we get:
$$2mc^2 h\nu = 0$$
−Since the electron mass $m \neq 0$, the speed of light $c \neq 0$, and Planck's constant $h \neq 0$, this equality holds true only if **$\nu = 0$**. Photons with zero frequency do not exist; therefore, complete absorption is impossible.
+Since the electron mass $m \neq 0$, the speed of light $c \neq 0$, and Planck's constant $h \neq 0$, this equality holds true only if $\nu = 0$. Photons with zero frequency do not exist; therefore, complete absorption is impossible.
<b>2. Impossibility of emission:</b>
Suppose a free electron at rest emits a photon with frequency $\nu$.
@@ -35,11 +29,7 @@Solution
The law of conservation of energy is:
$$mc^2 = \sqrt{\left(-\frac{h\nu}{c}\right)^2 c^2 + m^2 c^4} + h\nu$$
$$mc^2 = \sqrt{(h\nu)^2 + m^2 c^4} + h\nu$$
−Since $h\nu > 0$, the right side of the equation is always strictly greater than $mc^2$. The equality is possible only if **$\nu = 0$** (meaning no emission occurs).
+Since $h\nu > 0$, the right side of the equation is always strictly greater than $mc^2$. The equality is possible only if $\nu = 0$ (meaning no emission occurs).
#### Answer
The simultaneous satisfaction of the laws of conservation of energy and momentum during the absorption or emission of a photon by a free electron is possible only if the photon frequency is $\nu = 0$. Such photons do not exist.
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−#### Answer
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−[Insert a concise answer or boxed result]