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. 1999 Feb 16;96(4):1193–1200. doi: 10.1073/pnas.96.4.1193

Table 1.

Spectroscopic and photolytic characteristics of cage compounds

Cmpd λabs ɛ(λabs) ɛ(365) ɛ(400) Qu1 ɛQu1(365) Qf1 λem δf(740) δf(800) δu(740) δu(800)
1* 262 5,100 180 0.14 25 ∼0
2 345 5,900* 4,900 1,050 0.006 29 ∼0
3 346 6,100 5,200 1,300 0.005 26 ∼0 0.03 0.01
4 325 11,600 4,100 1,000 0.025 103 0.20 474 3.85 ± 0.31 1.26 ± 0.04 1.07 ± 0.05 0.13 ± 0.01
5 370 16,000 15,900 5,000 0.01 302 0.37 474 9.68 ± 0.32 3.22 ± 0.09 1.07 ± 0.07 0.34 ± 0.02
6 370 15,000 14,800 5,000 0.037 548 0.22 474 4.24 ± 0.12 1.41 ± 0.05 1.99 ± 0.09 0.42 ± 0.01
7 397 15,900 9,700 15,700 0.065 630 0.16 498 0.96 ± 0.05 3.1 ± 0.2
8 369 19,550 19,200 7,560 0.019 364 0.89 ± 0.24 0.42 ± 0.11
9 368 17,470 17,300 5,400 0.019 329 0.38 474 2.2 0.95 ± 0.21 0.37 ±0.06

λabs, wavelength in nm of absorbance maximum, ɛ, extinction coefficient in M−1 cm−1 at wavelength indicated; Qu1, quantum efficiency for uncaging with one-photon excitation at 365 nm; Qf1, quantum efficiency for fluorescence with one-photon excitation; λem, wavelength in nm for fluorescence emission peak; δf, fluorescence action cross section in 10−50 cm4 s/photon for two-photon excitation at wavelength indicated (δf = δaQf2, where δa is the absorbance cross section and Qf2 is the quantum efficiency for fluorescence, both with two-photon excitation); δu, uncaging action cross section in GM (10−50 cm4 s/photon) for two-photon excitation at wavelength indicated (δu = δaQu2, where Qu2 is the quantum efficiency for uncaging with two-photon excitation). Measurements were made in KMops at 24–25°C. Error estimates are standard deviations. 

*Values taken from the literature (30, 31); For compound 1, the entries listed under ɛ(365) and ɛQu1(365) actually refer to 360 nm. 

δu could not be measured because breakdown was dominated by dark hydrolysis with a 19.8-h exponential time constant. 

Value was measured at 780 nm on an independent apparatus.