物理化学学报
物理化學學報
물이화학학보
ACTA PHYSICO-CHIMICA SINICA
2009年
3期
423-429
,共7页
曹振洲%张昌华%王艳梅%张锋%华林强%张冰
曹振洲%張昌華%王豔梅%張鋒%華林彊%張冰
조진주%장창화%왕염매%장봉%화림강%장빙
离子速度影像%光解离%邻溴甲苯
離子速度影像%光解離%鄰溴甲苯
리자속도영상%광해리%린추갑분
Ion velocity imaging%Photodissociation%o-Bromotoluene
利用离子速度影像技术结合共振增强多光子电离(REMPI)技术,研究了邻溴甲苯在234和267 nm激光作用下的光解机理.平动能分布表明,基态Br(2P3/2和自旋轨道激发态Br(2>P3/2)产生于两个解离通道:快通道和慢通道.快通道的各向异性参数在234 nm分别为1.15(Br)和0.55(Br*),在267nm分别为0.90(Br)和0.60(Br*).慢通道的各向异性参数在234nm分别为0.12(Br)和0.14(Br*),在267nm分别为0.11(Br)和0.10(Br*).源自于慢通道的Br和Br*碎片的各向异性弱于快通道.Br(2P3/2)的相对量子产率φ(Br)在234 nm为0.67,在267 nm为0.70.邻溴甲苯在234和267 nm光解主要产生基态产物Br(2P3/2).快通道产生于(π,π*)束缚单重态被激发,随后通过排斥性(n,σ)态的预解离.慢通道各向异性参数接近零,由此证实慢通道来源于单重激发态内转换到高振动基态而引发的热解离.
利用離子速度影像技術結閤共振增彊多光子電離(REMPI)技術,研究瞭鄰溴甲苯在234和267 nm激光作用下的光解機理.平動能分佈錶明,基態Br(2P3/2和自鏇軌道激髮態Br(2>P3/2)產生于兩箇解離通道:快通道和慢通道.快通道的各嚮異性參數在234 nm分彆為1.15(Br)和0.55(Br*),在267nm分彆為0.90(Br)和0.60(Br*).慢通道的各嚮異性參數在234nm分彆為0.12(Br)和0.14(Br*),在267nm分彆為0.11(Br)和0.10(Br*).源自于慢通道的Br和Br*碎片的各嚮異性弱于快通道.Br(2P3/2)的相對量子產率φ(Br)在234 nm為0.67,在267 nm為0.70.鄰溴甲苯在234和267 nm光解主要產生基態產物Br(2P3/2).快通道產生于(π,π*)束縳單重態被激髮,隨後通過排斥性(n,σ)態的預解離.慢通道各嚮異性參數接近零,由此證實慢通道來源于單重激髮態內轉換到高振動基態而引髮的熱解離.
이용리자속도영상기술결합공진증강다광자전리(REMPI)기술,연구료린추갑분재234화267 nm격광작용하적광해궤리.평동능분포표명,기태Br(2P3/2화자선궤도격발태Br(2>P3/2)산생우량개해리통도:쾌통도화만통도.쾌통도적각향이성삼수재234 nm분별위1.15(Br)화0.55(Br*),재267nm분별위0.90(Br)화0.60(Br*).만통도적각향이성삼수재234nm분별위0.12(Br)화0.14(Br*),재267nm분별위0.11(Br)화0.10(Br*).원자우만통도적Br화Br*쇄편적각향이성약우쾌통도.Br(2P3/2)적상대양자산솔φ(Br)재234 nm위0.67,재267 nm위0.70.린추갑분재234화267 nm광해주요산생기태산물Br(2P3/2).쾌통도산생우(π,π*)속박단중태피격발,수후통과배척성(n,σ)태적예해리.만통도각향이성삼수접근령,유차증실만통도래원우단중격발태내전환도고진동기태이인발적열해리.
The photedissociation of o-bromotoluene was studied at 234 and 267 nm using velocity map imaging combined with a resonance-enhanced multiphoton ionization (REMPI) technique. Translational energy distributions suggested that ground state Br(2P3/2) and spin-orbit excited state Br*(2P3/2) fragments were all generated via two dissociation channels: a fast channel and a slow channel. The anisotropy parameters of the fast channels were determined to be 1.15 (Br) and 0.55 (Br*) at 234 am, 0.90 (Br) and 0.60 (Br*) at 267 am. The anisotropy parameters of the slow channels were 0.12 (Br) and 0.14 (Br*) at 234 am, 0.11 (Br) and 0.10 (Br*) at 267 am. The Br and Br* fragments of the slow channel were less anisotropic than those of the fast channel. The total relative quantum yields of Br (φ(Br)) were 0.67 at 234 nm and 0.70 at 267 run. Ground state Br(2P,3/2) was the main product from the photolysis of o-bromotoluene at 234 and 267 am. We propose that the fast channel originates from excitation of bound excited singlet (π,π*)states followed bypredissociation along repulsive (n,σ*) states. The anisotropy parameters of the slow channels were close to zero indicating a hot dissociation mechanism on a highly vibrational ground state followed the internal conversion of the excited singlet state.