Units & Conversions — Abridged Guide

Quick-reference equations, tables, and rules of thumb for photonics unit conversions. For full derivations, worked examples, and diagrams, see the Comprehensive Guide.

1.Overview

Photonics uses multiple unit systems because different subfields describe the same physical phenomena in different ways: wavelength (nm) in laser optics, frequency (THz) in RF/telecom, wavenumber (cm⁻¹) in spectroscopy, and photon energy (eV) in semiconductor physics.
Key constants: c=2.998×108 m/sc = 2.998 \times 10^8 \text{ m/s}, h=6.626×1034 J\cdotpsh = 6.626 \times 10^{-34} \text{ J·s}, hc=1240 eV\cdotpnmhc = 1240 \text{ eV·nm} (memory shortcut).

2.SI Prefixes

PrefixSymbolFactorPhotonics Use
femtof10⁻¹⁵fs (pulse widths)
picop10⁻¹²ps (pulse widths), pW (detector NEP)
nanon10⁻⁹nm (wavelength), nrad (pointing)
microµ10⁻⁶µm (IR wavelength), µrad (divergence), µW
millim10⁻³mm (optic sizes), mrad (divergence), mW
kilok10³kHz (rep rate), kW (fiber lasers)
megaM10⁶MHz (rep rate), MW (peak power)
gigaG10⁹GHz (FSR, linewidth), GW (peak power)
teraT10¹²THz (optical frequency)
Most common in optics: nm for wavelength (UV-Vis-NIR), µm for IR/telecom, mrad for beam divergence, fs/ps for ultrafast pulse widths.

3.Wavelength, Frequency & Wavenumber

Wavelength ↔ Frequency
λ=cνν=cλ\lambda = \frac{c}{\nu} \qquad \nu = \frac{c}{\lambda}
Wavenumber (Spectroscopic)
ν~=1λ=νc[cm1]\tilde{\nu} = \frac{1}{\lambda} = \frac{\nu}{c} \quad \text{[cm}^{-1}\text{]}
Use λ in cm: 532 nm = 5.32 × 10⁻⁵ cm → ν̃ = 18,797 cm⁻¹
Quick Conversions
λ (nm)=107ν~ (cm1)ν (THz)=cλ (µm)299.79λ (µm)\lambda \text{ (nm)} = \frac{10^7}{\tilde{\nu} \text{ (cm}^{-1}\text{)}} \qquad \nu \text{ (THz)} = \frac{c}{\lambda \text{ (µm)}} \approx \frac{299.79}{\lambda \text{ (µm)}}
Laserλ (nm)ν (THz)ν̃ (cm⁻¹)
ArF excimer193155351,813
Nd:YAG 2ω532563.518,797
HeNe632.8473.815,803
Nd:YAG 1ω1064281.89,398
CO₂10,60028.3943

4.Photon Energy

Planck's Relation
E=hν=hcλE = h\nu = \frac{hc}{\lambda}
The 1240 Rule
E (eV)=1240λ (nm)λ (nm)=1240E (eV)E \text{ (eV)} = \frac{1240}{\lambda \text{ (nm)}} \qquad \lambda \text{ (nm)} = \frac{1240}{E \text{ (eV)}}
Works because hc ≈ 1240 eV·nm (exact: 1239.842)
Shorter wavelength = higher photon energy. UV photons carry enough energy to break chemical bonds (>3 eV), while IR photons primarily cause molecular vibrations (<1 eV).

5.Power, Energy & Photon Flux

CW Power
P=Et=Φphcλ    [W]P = \frac{E}{t} = \Phi_p \cdot \frac{hc}{\lambda} \;\; \text{[W]}
P = power, Φₚ = photon flux (photons/s)
Photon Flux
Φp=Pλhc=5.034×1015×P(W)×λ(nm)    [photons/s]\Phi_p = \frac{P\lambda}{hc} = 5.034 \times 10^{15} \times P\,(\text{W}) \times \lambda\,(\text{nm}) \;\; \text{[photons/s]}
Longer wavelength = more photons per watt (each photon carries less energy). A 1 W source at 1550 nm produces ~6× more photons/s than a 1 W source at 250 nm.
For pulsed laser quantities (peak power, fluence, pulse energy scaling), see the Pulsed Lasers guide.

6.Radiometric Units

Radiometry measures electromagnetic radiation physically, across all wavelengths.

QuantitySymbolSI UnitMeaning
Radiant fluxΦₑWTotal optical power
Radiant intensityIₑW/srPower per solid angle
IrradianceEₑW/m²Power per area (incident)
Radiant exitanceMₑW/m²Power per area (emitted)
RadianceLₑW/(m²·sr)Power per area per solid angle
Solid Angle
Ω=Ar2  [sr]Cone: Ω=2π(1cosθ)Full sphere: 4π sr\Omega = \frac{A}{r^2} \;\text{[sr]} \qquad \text{Cone: } \Omega = 2\pi(1-\cos\theta) \qquad \text{Full sphere: } 4\pi \text{ sr}
"Intensity" is ambiguous. SI defines it as W/sr, but many optics texts use it for W/m². Always check the units on any datasheet specifying "intensity."
Radiance is conserved along a ray in a lossless medium — it is the fundamental quantity in radiative transfer.

7.Photometric Units

Photometry weights radiation by human visual response V(λ), peaking at 555 nm.

PhotometricSymbolSI UnitRadiometric Equiv.
Luminous fluxΦᵥlm (lumen)Radiant flux (W)
Luminous intensityIᵥcd (candela)Radiant intensity (W/sr)
IlluminanceEᵥlx (lux)Irradiance (W/m²)
LuminanceLᵥcd/m² (nit)Radiance (W/m²/sr)
Luminous Efficacy
K(λ)=683×V(λ)    [lm/W]K(\lambda) = 683 \times V(\lambda) \;\;\text{[lm/W]}
Maximum 683 lm/W at 555 nm. At 532 nm: 589 lm/W. At 635 nm: 148 lm/W.
A 5 mW green (532 nm) laser pointer produces ~2.9 lumens — 4× brighter to the eye than a 5 mW red (635 nm) pointer at ~0.74 lumens, despite equal optical power.

8.Radiometric ↔ Photometric Conversion

General Conversion (Broadband)
Xv=683380780Xe,λ(λ)V(λ)dλX_v = 683 \int_{380}^{780} X_{e,\lambda}(\lambda)\,V(\lambda)\,d\lambda
Monochromatic Shortcut
Φv=683×V(λ0)×Φe\Phi_v = 683 \times V(\lambda_0) \times \Phi_e
Works for any corresponding pair (irradiance → illuminance, etc.)
Photometric units are meaningless for UV and IR. V(λ) = 0 outside 380–780 nm, so a 10 W CO₂ laser (10.6 µm) has exactly zero lumens. Use radiometric units for non-visible radiation.
Use CaseSystemWhy
Laser powerRadiometric (W)Physical energy
Detector specRadiometric (A/W)Wavelength-dependent
Room lightingPhotometric (lux)Human comfort
Display brightnessPhotometric (nit)Perceived brightness
UV/IR sourcesRadiometric onlyNo visual response

9.Angular & Spatial Units

Radian ↔ Degree
1 rad=57.296°1°=0.01745 rad1°=60=36001 \text{ rad} = 57.296° \qquad 1° = 0.01745 \text{ rad} \qquad 1° = 60' = 3600''
Milliradian Conversions
1 mrad=0.0573°=3.44=206.31 rad=2062651 \text{ mrad} = 0.0573° = 3.44' = 206.3'' \qquad 1 \text{ rad} = 206\,265''
Beam divergence is specified in mrad. Pointing stability is specified in µrad. One µrad = 1 µm displacement per 1 m distance.
Small-angle approximation: sinθtanθθ\sin\theta \approx \tan\theta \approx \theta (in radians) for θ10°\theta \lesssim 10°. This underpins all of paraxial optics.

10.Practical Conversion Reference

Laserλ (nm)ν (THz)ν̃ (cm⁻¹)E (eV)
ArF excimer193155351,8136.424
KrF excimer248120940,3235.000
Ar-ion488614.520,4922.541
Nd:YAG 2ω532563.518,7972.331
HeNe632.8473.815,8031.960
Ti:Sapph800374.712,5001.550
Nd:YAG 1ω1064281.89,3981.165
Er:fiber1550193.46,4520.800
CO₂10,60028.27943.40.117
ImperialMetricContext
¼"-20 threadM6 × 1.0Posts, holders, table mount
8-32 threadM4 × 0.7Small components, cage
1" optic Ø25.4 mmStandard optic/mount
½" optic Ø12.7 mmCompact/cage system
2" optic Ø50.8 mmLarge aperture
Temperature
T(K)=T(°C)+273.15T(°F)=95T(°C)+32T(K) = T(°C) + 273.15 \qquad T(°F) = \tfrac{9}{5}\,T(°C) + 32
Key lengths: 1 inch = 25.4 mm (exact). 1 Å = 0.1 nm. Room temperature ≈ 20–25 °C = 293–298 K. Standardise on one thread system (¼-20 or M6) per lab — never mix.
Continue Learning

The Comprehensive Guide includes 6 worked examples, SVG diagrams, full explanations of radiometric and photometric systems, and detailed derivations for every formula on this page.

All information, equations, and calculations have been compiled and verified to the best of our ability. For mission-critical applications, we recommend independent verification of all values. If you find an error, please let us know.