TY - JOUR
T1 - Adsorption of nitric oxide on Ir{100}: Influence of substrate reconstruction
AU - Gardner, P.
AU - Martin, R.
AU - Nalezinski, R.
AU - Lamont, C. L A
AU - Weaver, M. J.
AU - Bradshaw, A. M.
PY - 1995
Y1 - 1995
N2 - We present a detailed study of the interaction of nitric oxide (NO) with the reconstructed (5 × 1) and metastable (1 × 1) surfaces of Ir{100} using vibrational spectroscopy and low-energy electron diffraction (LEED). Despite certain similarities with the corresponding Pt system, for example in the adsorbate-induced lifting of the reconstruction, the temperature-dependent adsorption behaviour in the present case in much more complex. In particular, dissociation plays an important role. On the (1 × 1) phase molecular adsorption takes place at low temperature, giving rise to characteristic N - O stretching bands in the regions 1570-1700 cm-1 and 1800-1870 cm-1. At 300 K, however, molecular adsorption only occurs after formation of a p(2 × 2) structure due to atomic oxygen (and perhaps atomic nitrogen). The resulting overlayer is structurally rather complicated, showing both half-order and sixth-order features in LEED. Desorption and/or further dissociation of the molecular NO produces a sharp p(2 × 1) pattern due to atomic oxygen with a coverage of Θo = 0.5. In contrast to the (1 × 1) surface the initial adsorption of NO on the (5 × 1) surface is molecular at all temperatures, indicating the lower reactivity of the more closely packed pseudo-hexagonal surface towards dissociation. The reconstruction is not lifted immediately at 300 K, but only after a significant coverage of molecular NO has been reached; the adsorbate-induced phase change still occurs at 90 K, but somewhat less readily. This represents another interesting difference compared with Pt{100} where the lifting of the (hex) phase reconstruction is immediate above 200 K.
AB - We present a detailed study of the interaction of nitric oxide (NO) with the reconstructed (5 × 1) and metastable (1 × 1) surfaces of Ir{100} using vibrational spectroscopy and low-energy electron diffraction (LEED). Despite certain similarities with the corresponding Pt system, for example in the adsorbate-induced lifting of the reconstruction, the temperature-dependent adsorption behaviour in the present case in much more complex. In particular, dissociation plays an important role. On the (1 × 1) phase molecular adsorption takes place at low temperature, giving rise to characteristic N - O stretching bands in the regions 1570-1700 cm-1 and 1800-1870 cm-1. At 300 K, however, molecular adsorption only occurs after formation of a p(2 × 2) structure due to atomic oxygen (and perhaps atomic nitrogen). The resulting overlayer is structurally rather complicated, showing both half-order and sixth-order features in LEED. Desorption and/or further dissociation of the molecular NO produces a sharp p(2 × 1) pattern due to atomic oxygen with a coverage of Θo = 0.5. In contrast to the (1 × 1) surface the initial adsorption of NO on the (5 × 1) surface is molecular at all temperatures, indicating the lower reactivity of the more closely packed pseudo-hexagonal surface towards dissociation. The reconstruction is not lifted immediately at 300 K, but only after a significant coverage of molecular NO has been reached; the adsorbate-induced phase change still occurs at 90 K, but somewhat less readily. This represents another interesting difference compared with Pt{100} where the lifting of the (hex) phase reconstruction is immediate above 200 K.
U2 - 10.1039/FT9959103575
DO - 10.1039/FT9959103575
M3 - Article
SN - 0956-5000
VL - 91
SP - 3575
EP - 3584
JO - Journal of the Chemical Society - Faraday Transactions
JF - Journal of the Chemical Society - Faraday Transactions
IS - 20
ER -