Zhong-Jun Zhou

Exceptionally Large Second-Order Nonlinear Optical Response in Donor–Graphene Nanoribbon–Acceptor Systems

Graphene nanoribbon (GNR) has been used, for the first time, as an excellent conjugated bridge in a donor-conjugated bridge-acceptor (D-B-A) framework to design high-performance second-order nonlinear optical materials. Owing to the unique diradical planar conjugated bridge of GNR, D(NH(2))-GNR-A(NO(2)) exhibits exceptionally large static first hyperpolarizability (β(0)) up to 2.5×10(6) a.u. (22000×10(-30) esu) for H(2)N-(7,3)ZGNR-NO(2) (ZGNR=zigzag-edged GNR), which is about 15 times larger than the recorded value of β(0) (1470×10(-30) esu) for the D-A polyene reported by Blanchard-Desce et al. [Chem. Eur. J. 1997, 3, 1091]. Interestingly, we have found that the size effect of GNR plays a key role in increasing β(0) for the H(2)N-GNR-NO(2) system, in which the width effect of GNR perpendicular to the D-A direction is superior to the length effect along the D-A direction.

New acceptor-bridge-donor strategy for enhancing NLO response with long-range excess electron transfer from the NH2...M/M3O donor (M = Li, Na, K) to inside the electron hole cage C20F19 acceptor through the unusual σ chain bridge (CH2)4.

Using the strong electron hole cage C20F19 acceptor, the NH2...M/M3O (M = Li, Na, and K) complicated donors with excess electron, and the unusual σ chain (CH2)4 bridge, we construct a new kind of electride molecular salt e(-)@C20F19-(CH2)4-NH2...M(+)/M3O(+) (M = Li, Na, and K) with excess electron anion inside the hole cage (to be encapsulated excess electron-hole pair) serving as a new A-B-D strategy for enhancing nonlinear optical (NLO) response. An interesting push-pull mechanism of excess electron generation and its long-range transfer is exhibited. The excess electron is pushed out from the (super)alkali atom M/M3O by the lone pair of NH2 in the donor and further pulled inside the hole cage C20F19 acceptor through the efficient long σ chain (CH2)4 bridge. Owing to the long-range electron transfer, the new designed electride molecular salts with the excess electron-hole pair exhibit large NLO response. For the e(-)@C20F19-(CH2)4-NH2...Na(+), its large first hyperpolarizability (β0) reaches up to 9.5 × 10(6) au, which is about 2.4 × 10(4) times the 400 au for the relative e(-)@C20F20...Na(+) without the extended chain (CH2)4-NH2. It is shown that the new strategy is considerably efficient in enhancing the NLO response for the salts. In addition, the effects of different bridges and alkali atomic number on β0 are also exhibited. Further, three modulating factors are found for enhancing NLO response. They are the σ chain bridge, bridge-end group with lone pair, and (super)alkali atom. The new knowledge may be significant for designing new NLO materials and electronic devices with electrons inside the cages. They may also be the basis of establishing potential organic chemistry with electron-hole pair.

The interaction between superalkalis (M3O, M = Na, K) and a C20F20 cage forming superalkali electride salt molecules with excess electrons inside the C20F20 cage: dramatic superalkali effect on the nonlinear optical property

It is well known that electrides are a type of multielectron many-cage solid salt with excess electron anions inside the cages. The main concern regarding these structures is how to construct the organic single-caged electride molecules with an electron inside its cage. Using the perfluorinated fullerene cage C20F20 as the electron hole, the alkali metal atoms (M = Na, K) and superalkali atoms (M3O, M = Na, K) with a smaller vertical detachment energy (VDE) value as the source of the electrons, we can construct new nonlinear optical (NLO) organic single-caged electride salt molecules M+(e@C20F20)− and (M3O)+(e@C20F20)− due to the long-range charge transfer from the (super)alkali to inside the cage, forming an electron-hole pair within the molecule. To measure the nonlinear optical response, static first hyperpolarizabilities (β0) and the superalkali effect on β0 are exhibited for these new molecules. The β0 values are 400 and 600 au for M+(e@C20F20)− which are considerably smaller than 13 000 and 10 000 au for (M3O)+(e@C20F20)−. It is revealed that the superalkali effect on the β0 value is dramatic and the β0 value increases by about 20–30 times. New single-caged superalkali electride salt molecules (M3O)+(e@C20F20)− possess not only a large nonlinear optical property but also higher stability. They hold potential as high-performance nonlinear optical materials.

Electric field-driven acid-base chemistry: proton transfer from acid (HCl) to base (NH3/H2O).

It is well-known that single H3N-HCl and H2O-HCl acid-base pairs do not react to form the ion pairs, H4N(+)Cl(-) and H3O(+)Cl(-), in isolation. On the basis of ab initio method, we propose a physical method of external electric field (Eext) to drive the proton transfer from acid (HCl) to base (NH3/H2O). Our results show that when Eext along the proton-transfer direction achieves or exceeds the critical electric field (Ec), the proton transfer occurs, such as, the Ec values of proton transfer for H3N-HCl and H2O-HCl are 54 × 10(-4) and 210 × 10(-4) au, respectively. And the degree of the proton transfer can be controlled by modulating the strength of Eext. Furthermore, we estimate the inductive strength of an excess electron (Ee) equivalent to the Eext = 125 × 10(-4) au, which is greater than the Ec (54 × 10(-4) au) of NH3-HCl but less than the Ec (210 × 10(-4) au) of H2O-HCl. This explains well the anion photoelectron spectroscopy [Eustis et al. Science 2008, 319, 936] that an excess electron can trigger the proton transfer for H3N-HCl but not for H2O-HCl. On the basis of the above estimation, we also predict that two excess electrons can induce H2O-HCl to undergo the proton transfer and form the ion pair H3O(+)Cl(-).

Li2 trapped inside tubiform [n] boron nitride clusters (n=4-8): structures and first hyperpolarizability.

The geometries and electronic properties of tubiform [n] boron nitride clusters entrapping Li(2) (Li(2)@BN-cluster(n,0); n=4-8), obtained by doping BN-cluster(n,0) with Li(2) molecules, are investigated by means of DFT. The effects of tube diameter n on the dipole moment μ(0), static polarizability α(0), and first hyperpolarizability β(0) are elucidated. Both the dipole moment and polarizability increase with increasing tube diameter, whereas variation of the static first hyperpolarizability with tube diameter is not monotonic; β(0) follows the order 1612 (n=4)<3112 (n=5)<5534 (n=7)<8244 (n=6)<12,282 a.u. (n=8). In addition, the natural bond orbital (NBO) charges show that charge transfer takes place from the Li(2) molecule to the BN cluster, except for BN-cluster(8,0) with larger tube diameter. Since the large-diameter tubular BN-cluster(8,0) can trap the excess electrons of the Li(2) molecule, Li(2)@BN-cluster(8,0) can be considered to be a novel electride compound.

Reaction Mechanism of CH + C3H6: A Theoretical Study

A detailed theoretical study is performed at the B3LYP/6-311G(d,p) and G3B3 (single-point) levels as an attempt to explore the reaction mechanism of CH with C(3)H(6). It is shown that the barrierless association of CH with C(3)H(6) forms two energy-rich isomers CH(3)-cCHCHCH(2) (1), and CH(2)CH(2)CHCH(2) (4). Isomers 1 and 4 are predicted to undergo subsequent isomerization and dissociation steps leading to ten dissociation products P(1) (CH(3)-cCHCHCH + H), P(2) (CH(3)-cCCHCH(2) + H), P(3) (cCHCHCH(2) + CH(3)), P(4) (CH(3)CHCCH(2) + H), P(5) (cis-CH(2)CHCHCH(2) + H), P(6) (trans-CH(2)CHCHCH(2) + H), P(7) (C(2)H(4) + C(2)H(3)), P(8) (CH(3)CCH + CH(3)), P(9) (CH(3)CCCH(3) + H) and P(12) (CH(2)CCH(2) + CH(3)), which are thermodynamically and kinetically possible. Among these products, P(5), P(6), and P(7) may be the most favorable products with comparable yields; P(1), P(2), and P(3) may be the much less competitive products, followed by the almost negligible P(4), P(8), P(9), and P(12). Since the isomers and transition states involved in the CH + C(3)H(6) reaction all lie lower than the reactant, the title reaction is expected to be fast, which is consistent with the measured large rate constant in experiment. The present study may lead us to a deep understanding of the CH radical chemistry.

Electric Field Effects on the Intermolecular Interactions in Water Whiskers: Insight from Structures, Energetics, and Properties

Modulation of intermolecular interactions in response to external electric fields could be fundamental to the formation of unusual forms of water, such as water whiskers. However, a detailed understanding of the nature of intermolecular interactions in such systems is lacking. In this paper, we present novel theoretical results based on electron correlation calculations regarding the nature of H-bonds in water whiskers, which is revealed by studying their evolution under external electric fields with various field strengths. We find that the water whiskers consisting of 2-7 water molecules all have a chain-length dependent critical electric field. Under the critical electric field, the most compact chain structures are obtained, featuring very strong H-bonds, herein referred to as covalent H-bonds. In the case of a water dimer whisker, the bond length of the novel covalent H-bond shortens by 25%, the covalent bond order increases by 9 times, and accordingly the H-bond energy is strengthened by 5 times compared to the normal H-bond in a (H2O)2 cluster. Below the critical electric field, it is observed that, with increasing field strength, H-bonding orbitals display gradual evolutions in the orbital energy, orbital ordering, and orbital nature (i.e., from typical π-style orbital to unusual σ-style double H-bonding orbital). We also show that, beyond the critical electric field, a single water whisker may disintegrate to form a loosely bound zwitterionic chain due to a relay-style proton transfer, whereas two water whiskers may undergo intermolecular cross-linking to form a quasi-two-dimensional water network. Overall, these results help shed new insight on the effects of electric fields on water whisker formation.

Theoretical investigation of boron-doped lithium clusters, BLin (n = 3–6), activating CO2: an example of the carboxylation of C–H bonds

This work reports the first example of boron-doped lithium clusters, BLin, activating CO2. The investigation shows that a kind of novel BLin–CO2 (n = 2–6) complex (In) with bidentate double oxygen M(η2-O2C) coordination is obtained through the bimetal 2Li of BLin clusters binding to the two O atoms of CO2, and the structural integrities of BLin clusters are not destroyed. We find that the partial negative charge transfer from BLin to the π* orbital of CO2 leads to weakening of the CO bonds of CO2 and an active CO2 moiety, except for when n = 2. Further, we perform reactions between In (n = 3–6) and benzene to elucidate a novel alternative approach to direct carboxylation by inserting CO2 into C–H bonds. We find that the carboxylation of the C–H bond of benzene can be achieved through the transition states (TS) of C–C bond formation and H-atom-transfer from C to O via two H2O molecules acting as a H-transfer tunnel. Comparing the transition states of H-direct transfer and one H2O molecule assisting H transfer, two H2O molecules assisting H-transfer as a tunnel is shown to lower the barrier, due to this long H-bond bridge effectively easing the rotation of the dihedral angle between the C6H6 and CO2 moiety planes. Considering the whole free energy profile, BLi5 and BLi6 clusters are more feasible for the carboxylation of C–H bonds.

Intercage electron transfer driven by electric field in Robin-Day-type molecules.

A new class of isomers, namely, intercage electron-transfer isomers, is reported for fluorinated double-cage molecular anion e(-)@C(20)F(18)(NH)(2)C(20)F(18) with C(20)F(18) cages: 1 with the excess electron inside the left cage, 2 with the excess electron inside both cages, and 3 with the excess electron inside the right cage. Interestingly, the C(20)F(18) cages may be considered as two redox sites existing in a rare nonmetal mixed-valent (0 and -1) molecular anion. The three isomers with two redox sites may be the founding members of a new class of mixed-valent compounds, namely, nonmetal Robin-Day Class II with localized redox centers for 1 and 3, and Class III with delocalized redox centers for 2. Two intercage electron-transfers pathways involving transfer of one or half an excess electron from one cage to the other are found: 1) Manipulating the external electric field (-0.001 a.u. for 1→3 and -0.0005 a.u. for 1→2) and 2) Exciting the transition from ground to first excited state and subsequent radiationless transition from the excited state to another ground state for 1 and 3. For the exhibited microscopic electron-transfer process 1→3, 2 may be the transition state, and the electron-transfer barrier of 6.021 kcal mol(-1) is close to the electric field work of 8.04 kcal mol(-1).

Excess-electron-induced C–C bond formation in transformation of carbon dioxide

This study presents a new fixation method of CO2 through excess-electron-induced C–C bond formation using quantum chemical method. Because of active CO2−˙ with a distinct radical character at the carbon center, two divalent anion complexes [O2C–C6H6–CO2]2− (cis-II and trans-II) are obtained via C–C bond formation between the carbon atom of C6H6 and the carbon atom of CO2 in the process of CO2−˙ radical attacking on benzene molecule. Furthermore, the transformations of cis-II and trans-II are predicted. We found that the more favorable transformation is for cis-II. It can produce terephthalic and one H2 molecule via two H-atom elimination with the energy barrier of 35.70 kcal mol−1. Furthermore, we found that the formed hydrogen bond complex CO2–HCN did not reduce the energy barrier; however, it could reduce the energy of the transition state with respect to that of the reactant, due to it dispersing the charge of benzene ring.