A plane electromagnetic wave is propagating
along the direction
${{\widehat i + \widehat j} \over {\sqrt 2 }}$
, with its polarization
along the direction $\widehat k$ . The correct form of the
magnetic field of the wave would be (here B0
is an appropriate constant) :
${B_0}{{\widehat i - \widehat j} \over {\sqrt 2 }}\cos \left( {\omega t - k{{\widehat i + \widehat j} \over {\sqrt 2 }}} \right)$
${B_0}{{\widehat i + \widehat j} \over {\sqrt 2 }}\cos \left( {\omega t - k{{\widehat i + \widehat j} \over {\sqrt 2 }}} \right)$