Order moves the Bragg path ledger below, onto, and above equality. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

Low order misses the path equality

Plane spacing and wavelength stay fixed while order changes. The accepted bit comes only from the checked path comparison.

nλ=24=8 m  2d2d=26=12 m,accepted=0\begin{array}{c}n\lambda=2\cdot 4=8\ \mathrm{m}\ \ne\ 2d\\2d=2\cdot 6=12\ \mathrm{m},\quad accepted=0\end{array}
Bragg order row lowOrder changes the left side of the checked equality.d=6 mlambda=4 mn=2n*lambda=8 m2d=12 maccepted=0

Matching order closes the path equality

Plane spacing and wavelength stay fixed while order changes. The accepted bit comes only from the checked path comparison.

nλ=34=12 m = 2d2d=26=12 m,accepted=1\begin{array}{c}n\lambda=3\cdot 4=12\ \mathrm{m}\ =\ 2d\\2d=2\cdot 6=12\ \mathrm{m},\quad accepted=1\end{array}
Bragg order row matchOrder changes the left side of the checked equality.d=6 mlambda=4 mn=3n*lambda=12 m2d=12 maccepted=1

High order overshoots the path equality

Plane spacing and wavelength stay fixed while order changes. The accepted bit comes only from the checked path comparison.

nλ=44=16 m  2d2d=26=12 m,accepted=0\begin{array}{c}n\lambda=4\cdot 4=16\ \mathrm{m}\ \ne\ 2d\\2d=2\cdot 6=12\ \mathrm{m},\quad accepted=0\end{array}
Bragg order row highOrder changes the left side of the checked equality.d=6 mlambda=4 mn=4n*lambda=16 m2d=12 maccepted=0