de Broglie wavelength of electrons

In 1924 Louis de Broglie theorized that not only light posesses both wave and particle properties, but rather particles with mass - such as electrons - do as well. The wavelength of these 'material waves' - also known as the de Broglie wavelength - can be calculated from Planks constant h divided by the momentum p of the particle. In the case of electrons that is $$\lambda_{\text{de Broglie}} = \frac {h}{p_\text e}=\frac {h}{m_\text e\cdot v_\text e}$$ The acceleration of electrons in an electron beam gun with the acceleration voltage Va results in the corresponding de Broglie wavelength $$\lambda_{\text{de Broglie}} = \frac {h}{m_\text e\cdot \sqrt{2\cdot \frac{e}{m_\text e}\cdot V_{\text a}}}=\frac {h}{\sqrt{2\cdot m_\text e \cdot e\cdot V_{\text a}}}$$ Proof of the de Broglie hypothesis will be experimentally demonstrated with the help of an electron diffraction tube on the following pages.

For electons with acceleration voltage Va, the following constansts will be used to calculate the de Broglie wavelengths:
($h=6{.}6\cdot 10^{-34}\,\text J\cdot \text s$, $ m_{\text e}=9{.}1\cdot 10^{-31}\,\text{kg}$, $e=1{.}6\cdot 10^{-19}\,{\text C}$)
acceleartion voltage Vade Broglie wavelength $\lambda_{\text {de Broglie}}$
10 V$3{,}87\cdot 10^{-10}\,\text m $
100 V$1{,}22\cdot 10^{-10}\,\text m $
1000 V$3{,}87\cdot 10^{-11}\,\text m $
10000 V$1{,}22\cdot 10^{-11}\,\text m $
V${}$