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使用粒子模拟程序和蒙特卡罗方法研究了双束对射圆极化激光与超薄氘靶相互作用中氘氘聚变反应产生中子的过程. 研究发现, 由于净光压和横向不稳定性发展的差异, 激光电场矢量旋转方向和初始相对相位差对氘靶压缩及中子特性有重要影响. 选择相对相位差为0且电场矢量旋转方向相同的双束光, 可获得最高的中子产额; 而采用相对相位差为0.5π或1.5π且电场矢量旋转方向不同的对射光, 中子具有定向的空间分布. 对于强度为1.23 × 1021 W/cm2、脉宽为33 fs、相对相位差为0.5π的左旋光和右旋光, 可获得产额为8.5 × 104 n、强度为1.2 × 1019 n/s、脉宽为23 fs、前冲性较好且分布可调谐的脉冲中子源.Neutron production via D(d, n)3He nuclear reaction during the interaction of two counter-propagating circularly polarized laser pulses with ultra-thin deuterium target is investigated by particle-in-cell simulation and Monte Carlo method. It is found that the rotation direction and initial relative phase difference of laser electric field vector have important effects on deuterium foil compression and neutron characteristics. The reason is attributed to the net light pressure and the difference in transverse instability development. The highest neutron yield can be obtained by choosing two laser pulses with a relative phase difference of 0 and the same rotation direction of the electric field vector. When the relative phase difference is 0.5π or 1.5π and the rotation direction of electric field vector is different, the neutrons have a directional spatial distribution and the neutron yield only slightly decreases. For left-handed circularly polarized laser pulse and right-handed circularly polarized laser pulse, each with an intensity of 1.23 × 1021 W/cm2, a pulse width of 33 fs and a relative phase difference of 0.5π, it is possible to produce a pulsed neutron source with a yield of 8.5 × 104 n, production rate of 1.2 × 1019 n/s, pulse width of 23 fs and good forward direction as well as tunable spatial distribution. Comparing with photonuclear neutron source and beam target neutron source driven by ultraintense laser pulses, the duration of neutron source in our scheme decreases significantly, thereby possessing many potential applications such as neutron nuclear data measurement. Our scheme offers a possible method to obtain a compact neutron source with short pulse width, high production rate and good forward direction.
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Keywords:
- two counter-propagating laser pulses /
- relative phase difference /
- rotation direction of electric-field vector /
- pulsed neutron source
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图 1 双束对射圆极化激光与超薄氘靶相互作用示意图, 其中红色曲线包络代表右旋光, 蓝色曲线包括代表左旋光,
$ k $ 代表坡印亭矢量 (a)—(d) 代表一束右旋光与一束左旋光的情况(RCP+LCP); (e)—(h) 代表两束右旋光的情况(RCP+RCP), 从左至右初始相对相位差$ \Delta \phi $ 依次为$ 0, {\text{ }}0.5\pi , {\text{ }}\pi , {\text{ }}1.5\pi $ Fig. 1. Schematic diagram of two counter-propagating circularly polarized laser pulses interacting with ultrathin deuterium target: (a)–(d) The cases of a left-rotating light and a right-rotating light (RCP+LCP); (e)–(h) the cases of two right-rotating light (RCP+RCP). From left to right, the initial relative phase difference
$ \Delta \phi $ is$ 0, {\text{ }}0.5{\text{π }}, {\text{ }}\pi , {\text{ }}1.5\pi $ , respectively. Here, red and blue curves represent the right- and left-rotating light and$ k $ is Poynting vector.
图 2
$ t = 32{T_0} $ 时, 不同电场矢量$ {\boldsymbol{E}}_{\text{r}} $ 旋转方向和不同初始相对相位差$ (\Delta \phi = 0, {\text{ }}0.5\pi , {\text{ }}\pi , {\text{ }}1.5\pi ) $ 情况下, 电子((a)—(d)和(i)—(l))和D+离子((e)—(h)和(m)—(p))的密度空间分布, 其中(a)—(h)和(i)—(p)分别代表RCP+LCP和RCP+RCP的情况Fig. 2. Spatial distributions of both electrons ((a)–(d) and (i)–(l)) and ions ((e)–(h) and (m)–(p)) for different rotation direction of electric fields
$ {\boldsymbol{E}}_{\text{r}} $ and initial relative phase$ (\Delta \phi = 0, {\text{ }}0.5\pi , {\text{ }}\pi , {\text{ }}1.5\pi ) $ at$ t = 32{T_0} $ . Here, (a)—(h) and (i)—(p) represent the cases of RCP+LCP and RCP+RCP, respectively.
图 3 不同电场矢量
$ {{{\boldsymbol E}}_{\text{r}}} $ 旋转方向和不同初始相对相位差$ (\Delta \phi = 0, {\text{ }}0.5\pi , {\text{ }}\pi , {\text{ }}1.5\pi ) $ 情况下,$ t = 50{T_0} $ 时电子((a), (b))和D+离子((c), (d))的能谱分布 (a), (c) RCP+LCP; (b), (d) RCP+RCPFig. 3. Spectral distributions of (a), (b) electrons and (c), (d) ions for the cases of different rotation direction of the electric fields
$ {{{\boldsymbol E}}_{\text{r}}} $ of two counter-propagating laser pulses and their initial relative phase$ (\Delta \phi = 0, {\text{ }}0.5\pi , {\text{ }}\pi , {\text{ }}1.5\pi ) $ at$ t = 50{T_0} $ : (a), (c) RCP+LCP; (b), (d) RCP+RCP.
图 4 不同电场矢量
$ {{{\boldsymbol E}}_{\text{r}}} $ 旋转方向和不同初始相对相位差$ \Delta \phi $ 情况下,$ t = 32{T_0} $ 时刻的中子产生率$ {P_{\text{n}}} $ ((a)—(h))和$ t = 50{T_0} $ 时的总中子产额$ {N_{\text{n}}} $ 分布((i)—(p))Fig. 4. Spatial distributions of (a)–(h) neutron production rate
$ {P_{\text{n}}} $ at$ t = 32{T_0} $ and (i)–(p) total neutron yield$ {N_{\text{n}}} $ at$ t = 50{T_0} $ in the cases of different rotation direction of electric fields$ {{{\boldsymbol E}}_{\text{r}}} $ of two counter-propagating laser pulses and their initial relative phase$ \Delta \phi $ .
图 5 不同电场矢量
$ {{{\boldsymbol E}}_{\text{r}}} $ 旋转方向和不同初始相对相位差$ \Delta \phi $ 情况下, 中子产生率$ {P_{\text{n}}} $ ((a), (b))和总中子产额$ {N_{\text{n}}} $ ((c), (d))随时间的演化Fig. 5. Temporal evolutions of (a), (b) neutron production rate
$ {P_{\text{n}}} $ and (c), (d) total neutron yield$ {N_{\text{n}}} $ in the cases of different rotation direction of electric fields$ {{{\boldsymbol E}}_{\text{r}}} $ of two counter-propagating laser pulses and their initial relative phase$ \Delta \phi $ .
图 6 不同电场矢量
$ {{\boldsymbol{E}}_{\text{r}}} $ 旋转方向和不同初始相对相位差$ \Delta \phi $ 情况下,$ t = 50{T_0} $ 时的中子能谱 (a) RCP+LCP; (b) RCP+RCPFig. 6. Spectra of the emitted neutrons at
$ t = 50{T_0} $ in the cases of different rotation direction of the electric fields$ {{\boldsymbol{E}}_{\text{r}}} $ of two counter-propagating laser pulses and their initial relative phase$ \Delta \phi $ : (a) RCP+LCP; (b) RCP+RCP.
图 7 不同电场矢量
$ {{{E}}_{\text{r}}} $ 旋转方向和不同初始相对相位差$ \Delta \phi $ 情况下,$ t = 25{T_0} $ (a), (b)和$ t = 50{T_0} $ (c)和(d)时刻的中子角分布Fig. 7. Angular distributions of the accumulated neutrons at
$ t = 25{T_0} $ (a), (b) and$ t = 50{T_0} $ (c), (d) in the cases of different rotation direction of electric fields$ {{{E}}_{\text{r}}} $ of two counter-propagating laser pulses and their initial relative phase$ \Delta \phi $ . -
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