| 1. | Connector - induced optical conductor loss
连接器引起的光导损耗 |
| 2. | Induced optical conductor loss
引起的光导体损耗 |
| 3. | Connector optical conductor loss
连接器光导损耗 |
| 4. | Optical conductor loss
光导体损耗 |
| 5. | The calculation results have shown that when the angles of the center electrode and the grounds decrease , the effective index , the characteristic impedance , and the conductor loss all decrease
通过计算发现，随着中间电极角度和地电极角度增加，有效折射率、特征阻抗同时减小，导体损耗系数也随之减小。 |
| 6. | There is integrated theoretic calculation , simple field , eliminate the reference of tan to rs , but the result comes from two samples without the conclusion of the conductor loss of cylindrical cavity
但是这种方法的测试结果是两片超导膜的平均值,而且未考虑到金属腔的导体损耗和其它一些因素引入的误差。 |
| 7. | The results show that the thickness and the width of the electrode , electrode gap and the thickness of upper cladding have different effects on microwave effective index , characteristic and conductor loss . compromising structure must be adopted in practical design to gain perfect performance
结果表明:电极的厚度和宽度、电极间距以及上包层的厚度对微波有效折射率、特征阻抗和导体损耗的影响是不同的,在实际设计时应当综合考虑。 |
| 8. | In this modulator , coplanar strips ( cps ) are used as electrodes for they support balance mode propagation of microwave , and this is a desired merit for common optical modulator . due to the miniaturized dimensions , the metallization thickness is in the order of skin depth and the conductor losses are not negligible
虽然由于金属的趋肤效应，电场将集中在金属表面，但在40g以上的频率条件下，金属的厚度和趋肤深度在一个量级，而且此时调制器带宽受到限制的最大根源来源于金属电极的微波损耗。 |
| 9. | It has been shown by our calculations that conductor loss is greatly reduced under velocity matching with relatively thick coplanar waveguide electrodes and thick buffer layer , but the characteristic impedance can not match with that of the external circuit at the same time , and the modulation bandwidth is confined in this case
然后，用一般的椭圆积分计算了普通共面波导型调制器的有效折射率、特征阻抗和导体损耗系数。通过计算发现，采用厚电极和厚缓冲层结构，在实现速度匹配的情况下，可以大大减小导体损耗，但是由于阻抗不能同时满足匹配，调制带宽受到限制。 |
