The -space region of wave vectors up to a given magnitude is a disk of area . The -space area occupied by a single particle state is
where the factor of is due to the spin degeneracy . The number of states with wave vector magnitude smaller than is
-space is used extensively in solid state physics e.g. to visualize the energy bands of a material as a function of electron momentum. In position space, the position-energy dispersion would just be a probability blur.
#import "@preview/cetz:0.5.2": canvas, draw
#import draw: circle, content, line
#set page(width: auto, height: auto, margin: 8pt, fill: none)
#set text(size: 12pt)
#let x-range = 3
#let y-range = 3
#let ratio = 3 / 4
#canvas({
// Set up coordinate system
circle(
(0, 0),
radius: 2 / 3 * y-range,
stroke: blue,
fill: blue.lighten(80%),
fill-opacity: 0.2,
name: "fermi-circle",
)
for x in range(-x-range, x-range + 1) {
for y in range(-y-range, y-range + 1) {
circle((x, ratio * y), radius: 2pt, fill: black)
}
}
let arrow-style = (mark: (end: "stealth", fill: black))
let x-end = (x-range + 0.5, 0)
let y-end = (0, ratio * y-range + 0.5)
line((-x-range - 0.5, 0), x-end, ..arrow-style)
line((0, -ratio * y-range - 0.5), y-end, ..arrow-style, name: "y-axis")
content(x-end, $k_x$, anchor: "south-west")
content((rel: (.55, 0), to: "y-axis.end"), $k_y$, anchor: "north-east")
let spacing-arrow = (
mark: (symbol: "stealth", fill: black, scale: .3, offset: 0.1),
stroke: 0.7pt,
)
let x-start = (x-range - 1, -ratio * y-range)
let x-end = (x-range, -ratio * y-range)
line(x-start, x-end, ..spacing-arrow, name: "x-spacing")
content("x-spacing.mid", $2pi \/ L_x$, anchor: "north", padding: 0.2)
let y-start = (x-range, -ratio * y-range)
let y-end = (x-range, -ratio * y-range + ratio)
line(y-start, y-end, ..spacing-arrow, name: "y-spacing")
content("y-spacing.mid", $2pi \/ L_y$, anchor: "west", padding: 0.2)
// Add N(k) label
let angle = 130deg
let label-pos = (calc.cos(angle) * 2.4, calc.sin(angle) * 2.4)
content(label-pos, text(blue)[$N(k)$])
})