Reference
The Electromagnetic Spectrum
From quasi-DC fields below one hertz to gamma rays beyond 1024 Hz — every electromagnetic phenomenon is a different frequency of the same underlying field. This table gathers the bands, their boundaries, the technology that lives in each, and the propagation quirks that make them useful (or useless) for any given purpose.
How to use: jump between batches with the tabs, type into the search box to filter rows live, or click Show more on long cells to expand the full text. The table scrolls horizontally on narrow screens and the header stays pinned as you scroll.
| Frequency Range (Hz) | Band Name / Designation | Wavelength Range | Photon Energy | Common / Alternative Names & Sub-bands | Primary Applications & Uses | Example Technologies / Systems | Propagation / Atmospheric Notes | Regulatory / Allocation Notes | Special Notes / Fun Facts |
|---|---|---|---|---|---|---|---|---|---|
| 0 Hz (DC / static fields) to ~0.001 Hz |
Ultra-Low
DC / Static Geomagnetic Fields
|
Effectively infinite (planetary / interplanetary scale) | < 4 × 10^{-18} eV (4 aeV) | Direct current (DC) geomagnetic field, Earth's core dynamo field, steady magnetospheric field |
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Fluxgate magnetometers (e.g., on Swarm satellites), ground-based observatories (INTERMAGNET network), paleomagnetic core sampling | Static fields penetrate the entire Earth and atmosphere with negligible attenuation. No wave propagation — purely magnetostatic. | No regulatory allocation (natural phenomenon). Used freely in scientific and geophysical research worldwide. |
Generated by convective currents in Earth's molten outer core. Strength... Show moreGenerated by convective currents in Earth's molten outer core. Strength ~25–65 μT at surface. Reversals occur every ~200,000–300,000 years. Used to date geological records via paleomagnetism.
|
| 0.001 Hz – 0.01 Hz (1–10 mHz) |
Ultra-Low
Ultra-Low Frequency Micropulsations (Pc5 class)
|
~30,000,000 km – 3,000,000 km (planetary scale) | ~4 × 10^{-18} eV – 4 × 10^{-17} eV (4–40 aeV) | Pc5 pulsations, global magnetospheric cavity modes, solar-wind-driven ULF waves |
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SuperMAG global magnetometer array, GOES/ACE satellite magnetometers, USGS geomagnetic observatories | Magnetohydrodynamic (MHD) waves in the magnetosphere. Couple to ground via ionospheric currents. Extremely long wavelengths allow global propagation with minimal loss. | Natural signals only — no licensing required. Monitored by international geophysical networks. |
Driven by solar-wind pressure pulses and Kelvin-Helmholtz instability at the... Show moreDriven by solar-wind pressure pulses and Kelvin-Helmholtz instability at the magnetopause. Can induce GIC (geomagnetically induced currents) in power lines, causing blackouts (e.g., 1989 Quebec event).
|
| 0.01 Hz – 0.1 Hz (10–100 mHz) |
Ultra-Low
Ultra-Low Frequency Micropulsations (Pc4 class)
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~3,000,000 km – 300,000 km | ~4 × 10^{-17} eV – 4 × 10^{-16} eV (40–400 aeV) | Pc4 pulsations, compressional ULF waves |
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CARISMA magnetometer chain (Canada), IMAGE array (Europe), THEMIS spacecraft magnetometers | Primarily compressional and toroidal MHD waves. Reach ground through ionospheric Hall/Pedersen currents. Highly latitude-dependent. | Unregulated natural signals. Studied under international programs (IAGA, INTERMAGNET). |
Period range 10–100 seconds. Often observed during geomagnetic storms. Can... Show morePeriod range 10–100 seconds. Often observed during geomagnetic storms. Can resonate with field lines, transferring energy from solar wind to the magnetosphere.
|
| 0.1 Hz – 1 Hz (100 mHz – 1 Hz) |
Ultra-Low
Ultra-Low Frequency Micropulsations (Pc3 class)
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~300,000 km – 30,000 km | ~4 × 10^{-16} eV – 4 × 10^{-15} eV (0.4–4 feV) | Pc3 pulsations, upstream waves, foreshock waves |
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Ground magnetometer arrays (e.g., SAMBA, MACCS), Cluster and MMS spacecraft, Japanese geomagnetic observatories | Waves generated in the foreshock region travel sunward then couple into the magnetosphere. Reach ground with moderate attenuation. | Natural only. No spectrum allocation. |
Often linked to 30-second upstream waves from the bow shock.... Show moreOften linked to 30-second upstream waves from the bow shock. Strongest during high solar-wind speed periods.
|
| 1 Hz – 3 Hz |
Ultra-Low
Upper Ultra-Low / Lower Extremely-Low Frequency Micropulsations
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~30,000 km – 10,000 km | ~4 × 10^{-15} eV – 1.2 × 10^{-14} eV (4–12 feV) | Pc2 pulsations (border), sub-ELF geomagnetic variations, power-grid sub-harmonics |
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High-sensitivity SQUID magnetometers, induction coils at remote observatories, Schumann-resonance-adjacent monitoring stations | Still dominated by magnetospheric/ionospheric coupling. Wavelengths comparable to Earth radius — global-scale standing waves possible. | No allocation. Overlaps with the very bottom edge of the ITU ELF band (3–3000 Hz) but remains natural-signal dominated. |
This range marks the transition into the official ELF band... Show moreThis range marks the transition into the official ELF band (ITU defines ELF starting at 3 Hz). Some studies link ultra-low geomagnetic fluctuations to subtle effects on human brain alpha waves or animal navigation, though evidence remains debated.
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| EXAMPLE: 3 Hz – 30 Hz |
ELF/SLF/ULF
EXAMPLE: ELF (Extremely Low Frequency)
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EXAMPLE: 100,000 km – 10,000 km | EXAMPLE: 1.24 × 10⁻¹⁴ – 1.24 × 10⁻¹³ eV | EXAMPLE: ELF, Schumann band |
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EXAMPLE: Project ELF / ZEVS transmitters, large loop antennas | EXAMPLE: Earth–ionosphere waveguide; very low attenuation in seawater | EXAMPLE: Mostly military / scientific use; not commercially allocated |
EXAMPLE: Schumann resonances peak near 7.83 Hz. Show moreEXAMPLE: Schumann resonances peak near 7.83 Hz.
|
| EXAMPLE: 3 kHz – 30 kHz |
VLF/LF/MF
EXAMPLE: VLF (Very Low Frequency)
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EXAMPLE: 100 km – 10 km | EXAMPLE: 1.24 × 10⁻¹¹ – 1.24 × 10⁻¹⁰ eV | EXAMPLE: Myriametric waves, Band 4 |
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EXAMPLE: Massive grounded antennas, ferrite-loop receivers | EXAMPLE: Stable Earth–ionosphere waveguide; penetrates ~20 m of seawater | EXAMPLE: ITU Band 4; mixed military / aeronautical / time-signal allocations |
EXAMPLE: Replace with real data. VLF transmitters have antennas measured... Show moreEXAMPLE: Replace with real data. VLF transmitters have antennas measured in kilometres.
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| EXAMPLE: 3 MHz – 30 MHz |
HF
EXAMPLE: HF (High Frequency)
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EXAMPLE: 100 m – 10 m | EXAMPLE: 1.24 × 10⁻⁸ – 1.24 × 10⁻⁷ eV | EXAMPLE: Short wave, decametric waves, Band 7 |
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EXAMPLE: SSB transceivers, dipole / Yagi / log-periodic antennas, NVIS | EXAMPLE: Skywave via F-layer; strongly diurnal and solar-cycle dependent | EXAMPLE: Densely allocated by ITU; amateur sub-bands (80m–10m); WARC bands |
EXAMPLE: Replace with real data. Maximum Usable Frequency (MUF) tracks... Show moreEXAMPLE: Replace with real data. Maximum Usable Frequency (MUF) tracks the solar cycle.
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| EXAMPLE: 30 MHz – 300 MHz |
VHF/UHF
EXAMPLE: VHF (Very High Frequency)
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EXAMPLE: 10 m – 1 m | EXAMPLE: 1.24 × 10⁻⁷ – 1.24 × 10⁻⁶ eV | EXAMPLE: Metric waves, Band 8 |
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EXAMPLE: Yagi antennas, vertical whips, FM transceivers, SDRs | EXAMPLE: Mostly line-of-sight with slight diffraction; sporadic-E and tropo-ducting possible | EXAMPLE: ITU Band 8; nationally licensed broadcast and safety services |
EXAMPLE: Replace with real data. Tropospheric ducting can carry VHF... Show moreEXAMPLE: Replace with real data. Tropospheric ducting can carry VHF hundreds of km on rare nights.
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| EXAMPLE: 3 GHz – 30 GHz |
SHF/EHF/µwave
EXAMPLE: SHF (Super High Frequency) / Microwave
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EXAMPLE: 10 cm – 1 cm | EXAMPLE: 1.24 × 10⁻⁵ – 1.24 × 10⁻⁴ eV | EXAMPLE: Centimetric waves; IEEE C / X / Ku / K bands |
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EXAMPLE: Parabolic dishes, phased arrays, GaN/GaAs HEMTs, waveguides | EXAMPLE: Strict line-of-sight; rain fade above ~10 GHz; atmospheric absorption peaks | EXAMPLE: ITU Region allocations; ISM at 2.4 / 5.8 / 24 GHz; auctioned 5G bands |
EXAMPLE: Replace with real data. 60 GHz suffers ~15 dB/km... Show moreEXAMPLE: Replace with real data. 60 GHz suffers ~15 dB/km O₂ absorption — useful for short-range security.
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| EXAMPLE: 300 GHz – 3 THz |
THz / IR
EXAMPLE: Terahertz / Sub-millimetre
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EXAMPLE: 1 mm – 100 µm | EXAMPLE: 1.24 meV – 12.4 meV | EXAMPLE: T-rays, sub-mm waves, far-IR boundary |
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EXAMPLE: Quantum-cascade lasers, photoconductive antennas, bolometers, HEB mixers | EXAMPLE: Heavy water-vapour absorption; non-ionising; cannot penetrate metal or water | EXAMPLE: Largely unallocated above ~275 GHz; ITU footnote 5.565 lists passive services |
EXAMPLE: Replace with real data. Historically called the 'terahertz gap'... Show moreEXAMPLE: Replace with real data. Historically called the 'terahertz gap' due to lack of compact sources.
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| EXAMPLE: 430 THz – 770 THz |
Visible → γ
EXAMPLE: Visible Light
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EXAMPLE: 700 nm – 380 nm | EXAMPLE: 1.65 eV – 3.26 eV | EXAMPLE: Optical, VIS, light |
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EXAMPLE: LEDs, lasers, CMOS/CCD sensors, optical fibres (near-IR / vis) | EXAMPLE: Line-of-sight; scattered by aerosols; absorbed strongly in water at red end | EXAMPLE: Not radio-regulated; eye-safety covered by IEC 60825 laser classes |
EXAMPLE: Replace with real data. Visible band is roughly one... Show moreEXAMPLE: Replace with real data. Visible band is roughly one octave wide — frequency doubles violet → red.
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