论文标题
从驻波光脉冲中衍射强烈相互作用的分子玻色子凝结物
Diffraction of strongly interacting molecular Bose-Einstein condensate from standing wave light pulses
论文作者
论文摘要
我们研究了强粒子相互作用对$^6LI_2 $分子的玻色丝凝结物的衍射的影响,这是由远不受欢迎的光学常驻波的脉冲产生的周期性电势。对于短脉冲,我们观察到标准的Kapitza-Dirac衍射,由于相互作用依赖性损耗过程,衍射模式的对比度大大降低了,因此非常大的相互作用。对于更长的脉冲,衍射显示了撞击管和相干通道传输的物质波的特征。我们观察到时间演变的放缓,该时间演化管理由强度相互作用引起的动量模式的种群。简单的物理解释是放慢速度的是由静光波中形成物质波模式的自我互动引起的相移。简单的一维平均场模拟定性地捕获现象,但是为了定量再现实验结果,分子散射长度必须乘以4.2倍。此外,确定了相干衍射模式的互动依赖性降解的两种贡献:(i)晶格脉冲期间分子的陷阱损失,涉及将feshbach分子分离为游离原子中的自由原子,这是通过无线电频谱光谱谱和(II)在分开模量之间的(II)碰撞碰撞之间证实的。通过将衍射矩形重组为零摩托峰的衍射臂通过干预来确认这一点,从而去除了散射背景。
We study the effects of strong inter-particle interaction on diffraction of a Bose-Einstein condensate of $^6Li_2$ molecules from a periodic potential created by pulses of a far detuned optical standing wave. For short pulses we observe the standard Kapitza-Dirac diffraction, with the contrast of the diffraction pattern strongly reduced for very large interactions due to interaction dependent loss processes. For longer pulses diffraction shows the characteristic for matter waves impinging on an array of tubes and coherent channeling transport. We observe a slowing down of the time evolution governing the population of the momentum modes caused by the strong atom interaction. A simple physical explanation of that slowing down is the phase shift caused by the self-interaction of the forming matter wave patterns inside the standing light wave. Simple 1D mean field simulations qualitatively capture the phenomenon, however to quantitatively reproduce the experimental results the molecular scattering length has to be multiplied by factor of 4.2. In addition, two contributions to interaction-dependent degradation of the coherent diffraction patterns were identified: (i) in-trap loss of molecules during the lattice pulse, which involves dissociation of Feshbach molecules into free atoms, as confirmed by radio-frequency spectroscopy and (ii) collisions between different momentum modes during separation. This was confirmed by interferometrically recombining the diffracted momenta into the zero-momentum peak, which consequently removed the scattering background.