=== The 60 GHz Oxygen Resonances === Tretyakov, M. Yu, M. A. Koshelev, V. V. Dorovskikh, D. S. Makarov, and P. W. Rosenkranz. "60-GHz oxygen band: precise broadening and central frequencies of fine-structure lines, absolute absorption profile at atmospheric pressure, and revision of mixing coefficients." Journal of Molecular Spectroscopy 231, no. 1 (2005): 1-14. http://radiometrics.com/data/uploads/2012/11/Tretyakova_JMS_05.pdf more than 37 resonances: ||Quantum|| freq || a1 || a2 ||a3 || a5 || a6 || ||ID || GHz || || ||GHz/10⁵Pa||1/10⁵Pa||1/10⁵Pa|| || 1+||56.264774|| 543.4||0.014||1.703 || 0.3525||-0.0978|| || 3-||62.486253||1503.0||0.083||1.513 ||-0.4499|| 0.0844|| || 3+||58.446588||1442.1||0.083||1.491 || 0.6768||-0.1273|| || 5-||60.306056||2103.4||0.207||1.415 ||-0.6395|| 0.0699|| || 5+||59.590983||2090.7||0.207||1.408 || 0.6957||-0.0776|| || 7-||59.164204||2379.9||0.387||1.353 ||-0.6561|| 0.2309|| || 7+||60.434778||2438.0||0.386||1.339 || 0.6342||-0.2825|| || 9-||58.323877||2363.7||0.621||1.295 ||-0.1932|| 0.0436|| || 9+||61.150562||2479.5||0.621||1.292 || 0.1014||-0.0584|| || 11-||57.612486||2120.1||0.910||1.262 ||-0.5416|| 0.6056|| || 11+||61.800158||2275.9||0.910||1.263 || 0.5014||-0.6619|| || 13-||56.968211||1746.6||1.255||1.223 ||-0.3545|| 0.6451|| || 13+||62.411220||1915.4||1.255||1.217 || 0.3029||-0.6759|| || 15-||56.363399||1331.8||1.654||1.189 ||-0.2378|| 0.6547|| || 15+||62.997984||1490.2||1.654||1.174 || 0.1856||-0.6675|| || 17-||55.783815|| 945.3||2.109||1.134 ||-0.1172|| 0.6135|| || 17+||63.568526||1078.0||2.108||1.134 || 0.0658||-0.6139|| || 19-||55.221384|| 627.1||2.618||1.089 || 0.2560|| 0.2952|| || 19+||64.127775|| 728.7||2.617||1.088 ||-0.3036||-0.2895|| || 21-||54.671180|| 389.7||3.182||1.037 || 0.3558|| 0.2654|| || 21+||64.678910|| 461.3||3.181||1.038 ||-0.3968||-0.2590|| || 23-||54.130025|| 227.3||3.800||0.996 || 0.3170|| 0.3750|| || 23+||65.224078|| 274.0||3.800||0.996 ||-0.3528||-0.3680|| || 25-||53.595775|| 124.6||4.474||0.955 || 0.2227|| 0.5085|| || 25+||65.764779|| 153.0||4.473||0.955 ||-0.2548||-0.5002|| || 27-||53.066934|| 64.29||5.201||0.906 || 0.1349|| 0.6206|| || 27+||66.302096|| 80.40||5.200||0.906 ||-0.1660||-0.6091|| || 29-||52.542418|| 31.24||5.983||0.858 || 0.1388|| 0.6526|| || 29+||66.836834|| 39.80||5.982||0.858 ||-0.1680||-0.6393|| || 31-||52.021429|| 14.32||6.819||0.811 || 0.1667|| 0.6640|| || 31+||67.369601|| 18.56||6.818||0.811 ||-0.1956||-0.6475|| || 33-||51.503360|| 6.193||7.709||0.764 || 0.1947|| 0.6729|| || 33+||67.900868|| 8.172||7.708||0.764 ||-0.2216||-0.6545|| || 35-||50.987745|| 2.529||8.653||0.717 || 0.2246|| 0.680 || || 35+||68.431006|| 3.397||8.652||0.717 ||-0.2492||-0.660 || || 37-||50.474214|| 0.975||9.651||0.669 || 0.2566|| 0.685 || || 37+||68.960312|| 1.334||9.650||0.669 ||-0.2773||-0.665 || ||Quantum|| freq || a1 || a2 ||a3 || a5 || a6 || ||ID || GHz || || ||GHz/10⁵Pa||1/10⁵Pa||1/10⁵Pa|| * a1 is proportional to magnitude of the effect. the center is around 59.4 GHz. * All of these lines are "pressure broadened" - they are sharper and more resonant in thinner air. At full atmospheric pressure, they merge into one broad curve. I was hoping there was a way to take advantage of these resonances - perhaps for beam focusing, or even tailoring a signal to punch through this resonance to reach the ground. If this is possible, it is beyond what I can imagine.