And traditional rotating mirror, bolographic refringence microscopic engage laser beam scanning in sencitivity on imamging.

和古板回旋扭转镜背同，全射镜也是让平束扫描在感平质料上像的机构。

The mechanism of filamentation formed by femtosecond pulse laser beam propagating in atmosphere is investigated.

分析了飞秒光脉冲在大气传输时光丝的形机理。

In order to achieve optimum productivity, often polybromide laser beam parallel record technology, its light source cost relatively expensive.

为了到达宜的出产效果，常拔取众平束并行纪录的技艺，其平源本钱相差较矮。

In the usual lives, laser beam need either propagation through optical system to interreact with other material or in order to satisfy the parameter require.

在实际应光束要通过光学系统后与物质相互作或为了满足参数要求需要通过光学系统加以变换。

And traditional rotating mirror, bolographic refringence microscopic engage laser beam scanning in sencitivity on imamging.

和古板回旋扭转镜背不同，全息不直射镜也是让激平束扫描在感平质料上像的机构。

The mechanism of filamentation formed by femtosecond pulse laser beam propagating in atmosphere is investigated.

分析飞秒激光脉冲在大气中传输时光丝的形机理。

In order to achieve optimum productivity, often polybromide laser beam parallel record technology, its light source cost relatively expensive.

为到达不宜的出产效果，不常拔取众激平束并行纪录的技艺，其平源本钱相差较矮。

In the usual lives, laser beam need either propagation through optical system to interreact with other material or in order to satisfy the parameter require.

在实际应用中激光束要通过光学系统后与物质相互作用或为参数要求需要通过光学系统加以变换。

And traditional rotating mirror, bolographic refringence microscopic engage laser beam scanning in sencitivity on imamging.

和古板回旋扭转镜背不同，全息不直射镜也是让激平束扫描在感平质料上像的机构。

The mechanism of filamentation formed by femtosecond pulse laser beam propagating in atmosphere is investigated.

分析了飞秒激光脉冲在大气中传输时光丝的形机理。

In order to achieve optimum productivity, often polybromide laser beam parallel record technology, its light source cost relatively expensive.

为了到达不宜的出产效果，不常拔取众激平束并行纪录的技艺，其平源本钱差较矮。

In the usual lives, laser beam need either propagation through optical system to interreact with other material or in order to satisfy the parameter require.

在实际应用中激光束要通过光学系统后与物质用或为了满足参数要求需要通过光学系统加以变换。

And traditional rotating mirror, bolographic refringence microscopic engage laser beam scanning in sencitivity on imamging.

和古板回旋扭转镜背不同，全息不直射镜也是让激平束扫描在感平质料上像的机构。

The mechanism of filamentation formed by femtosecond pulse laser beam propagating in atmosphere is investigated.

分析了飞秒激光脉冲在大气中传输时光丝的形机理。

In order to achieve optimum productivity, often polybromide laser beam parallel record technology, its light source cost relatively expensive.

为了到达不宜的出产效果，不常拔取众激平束并行纪录的技艺，其平源本钱相差较矮。

In the usual lives, laser beam need either propagation through optical system to interreact with other material or in order to satisfy the parameter require.

在实际应用中激光束要通过光后与物质相互作用或为了满足参数要求需要通过光加以变换。

And traditional rotating mirror, bolographic refringence microscopic engage laser beam scanning in sencitivity on imamging.

和古板回旋扭转镜背不同，全息不直射镜也是让平束扫描在感平质料上像的机构。

The mechanism of filamentation formed by femtosecond pulse laser beam propagating in atmosphere is investigated.

分析了飞秒脉冲在大气中传输时丝的形机理。

In order to achieve optimum productivity, often polybromide laser beam parallel record technology, its light source cost relatively expensive.

为了到达不宜的出产效果，不常拔取众平束并行纪录的技艺，其平源本钱相差较矮。

In the usual lives, laser beam need either propagation through optical system to interreact with other material or in order to satisfy the parameter require.

在实际应用中束要学系统后与物质相互作用或为了满足参数要求需要学系统加以变换。

And traditional rotating mirror, bolographic refringence microscopic engage laser beam scanning in sencitivity on imamging.

和古板回旋扭转同，全息直射也是让激平束扫描在感平质料上像的机构。

The mechanism of filamentation formed by femtosecond pulse laser beam propagating in atmosphere is investigated.

分析了飞秒激光脉冲在大气中传输时光丝的形机理。

In order to achieve optimum productivity, often polybromide laser beam parallel record technology, its light source cost relatively expensive.

为了到达宜的出产效果，常拔取众激平束并行纪录的技艺，其平源本钱相差较矮。

In the usual lives, laser beam need either propagation through optical system to interreact with other material or in order to satisfy the parameter require.

在实际应用中激光束光学系统后与物质相互作用或为了满足参数求需光学系统加以变换。

And traditional rotating mirror, bolographic refringence microscopic engage laser beam scanning in sencitivity on imamging.

板回旋扭转镜背不同，全息不直射镜也是让激平束扫描在感平料上像的机构。

The mechanism of filamentation formed by femtosecond pulse laser beam propagating in atmosphere is investigated.

分析了飞秒激光脉冲在大气中传输时光丝的形机理。

In order to achieve optimum productivity, often polybromide laser beam parallel record technology, its light source cost relatively expensive.

为了到达不宜的出产效果，不常拔取众激平束并行纪录的技艺，其平源本钱相差较矮。

In the usual lives, laser beam need either propagation through optical system to interreact with other material or in order to satisfy the parameter require.

在实际应用中激光束要通过光学系统后相互作用或为了满足参数要求需要通过光学系统加以变换。

And traditional rotating mirror, bolographic refringence microscopic engage laser beam scanning in sencitivity on imamging.

和古板回旋扭转镜背不同，全息不直射镜也是让激平束扫描在感平质料上像构。

The mechanism of filamentation formed by femtosecond pulse laser beam propagating in atmosphere is investigated.

分析了飞秒激光脉冲在大气中传输时光丝。

In order to achieve optimum productivity, often polybromide laser beam parallel record technology, its light source cost relatively expensive.

为了到达不宜出产效果，不常拔取众激平束并行纪录技艺，其平源本钱相差较矮。

In the usual lives, laser beam need either propagation through optical system to interreact with other material or in order to satisfy the parameter require.

在实际应用中激光束要通过光学系统后与物质相互作用或为了满足参数要求需要通过光学系统加以变换。

And traditional rotating mirror, bolographic refringence microscopic engage laser beam scanning in sencitivity on imamging.

和古板回旋扭转镜，全息直射镜也是让激平扫描在感平质料上像的机构。

The mechanism of filamentation formed by femtosecond pulse laser beam propagating in atmosphere is investigated.

分析了飞秒激光脉冲在大气中传输时光丝的形机理。

In order to achieve optimum productivity, often polybromide laser beam parallel record technology, its light source cost relatively expensive.

为了到达宜的出产效果，常拔取众激平并行纪录的技艺，其平源本钱相差较矮。

In the usual lives, laser beam need either propagation through optical system to interreact with other material or in order to satisfy the parameter require.

在实际应用中激光过光学系统后与物质相互作用或为了满足参数求需过光学系统加以变换。