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. 2019 Dec 3;116(49):24420-24424.
doi: 10.1073/pnas.1910647116. Epub 2019 Nov 15.

Thermal reaction and luminescence of long-lived N 2D in N2 ice

Affiliations

Thermal reaction and luminescence of long-lived N 2D in N2 ice

Jen-Iu Lo et al. Proc Natl Acad Sci U S A. .

Abstract

Photochemistry of an N2 ice and thermal reaction of the irradiated sample were studied with vacuum-ultraviolet (VUV) light from a synchrotron. Concurrent detection of infrared absorption and visible emission spectra provide evidence for the generation of energetic products N (2D) and N (2P) atoms, N2 (A) molecule and linear-N3 (l-N3) radical after excitation of icy N2 at 121.6 nm. Irradiation at 190 nm is shown to be an effective way to eliminate the l-N3 radical. After the photolysis and photoelimination of the l-N3, we initiate synthesis of l-N3 via the thermal ramping of the sample in temperature range 3.5 to 20 K. In addition, the emission from the N (2D) atom was observed during the thermal ramping process. These behaviors indicate that a long-lived N (2Dlong) atom is generated in the VUV-photolyzed N2 ice. A comparison of the variations of the visible emission of N (2D) and the infrared absorption of l-N3 with time indicates that the long-lived N (2Dlong) dominated the thermal synthesis of l-N3 The results have enhanced suggestion and understanding of the conversion for nitrogen species in cold astrophysical environments with VUV irradiation.

Keywords: atomic N (2D); azide radical; icy N2; photochemistry; vacuum-UV radiation.

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Conflict of interest statement

The authors declare no competing interest.

Figures

Fig. 1.
Fig. 1.
(A) Scheme of energetics and transitions for excitation of icy N2 at 121.6 nm, 10.20 eV. (B) Scheme of energetics and generation l-N3 for excitation of icy N2 at 121.6 nm. (C) Scheme of N (2P) and N (2D) atoms relax to their lower states N (2D) and N (4S), respectively, through emissions. (D) During thermal ramping (marked with symbols ▲), scheme of conversion and reaction of N (2Dlong) atoms.
Fig. 2.
Fig. 2.
Experimental procedure related to the photon current of irradiation, temporal profiles of the N α-line and temperature of the N2 ice. The graphic trend in A shows photon currents (logarithmic scale) of irradiated light; the scatters show the time line of recording various spectra, in which the triangle(▼), circle (●) and star(★) indicate when recording spectra IR, iEm, and Em, respectively. B shows temporal profiles of the height of the atomic N α-line monitored at 522.6 nm; both temporal profiles of iEm-1 and iEm-4 are flat because of saturation of the charge-coupled device (CCD) detector. C shows the variation of temperature of the N2 ice.
Fig. 3.
Fig. 3.
Emission spectra during irradiation at 121.6 nm. A and B are spectra of the 1st (recorded at 157 min) and 45th (recorded at 194 min) measured spectra in series spectra of iEm-1; both are labeled as iEm-1.1” and “iEm-1.45,” respectively. C indicates the 7th spectrum (recorded at 607 min) in series spectra of iEm-4; it is labeled as “iEm-4.7”. The notations “N2 VK” and “N2 VK, 2nd” represent the first- and second-order lines of N2 VK transition (26). The notations N (α) and N (α′) indicate lines of (0,0) and (0,1) from transitions N (2D → 4S), whereas N (δ) and N (δ″) indicate lines of (0,0) and (n,n-1) from transitions N (2P →2D) (26). The notation O (β) represents lines due to O (1S → 1D) from impurity O2.
Fig. 4.
Fig. 4.
Profiles of emissions near N α-line region for spectra iEm-# and Em-#. The iEm-# were the 1st of serial emission spectra, in which iEM-1 to iEM-5 were recorded at 155, 222, 497, 600, and 637 min, respectively. Em-# were averaged spectra from serial emission spectra, in which the 1st spectra of Em-1 to Em-4 were recorded at 354, 412, 456, and 550 min, respectively.
Fig. 5.
Fig. 5.
IR absorption spectra. The labels are those used in Fig. 1; the direct times of IR-1 to IR-8 were recorded at 142, 208, 300, 495, 540, 590, 630, and 710 min, respectively. The IR-1 is the spectrum of precursor N2 before irradiation, the IR-2 is the spectrum after irradiated 121.6 nm, the IR-3 is the spectrum after irradiated 190 nm, the IR-4 is the spectrum after thermal ramping, the IR-5 is the spectrum after irradiated 190 nm again, the IR-6 is the spectrum after thermal ramping again, the IR-7 is the spectrum after irradiated 121.6 nm again, and the IR-8 is the spectrum after irradiated 190 nm finally. The area ratios are among IR-2: IR-4: IR-5: IR-6: IR-7: IR-8 = 33: 7.8: 2: 3: 22: 1.

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