A 45nm SOI CMOS Class-D mm-Wave PA with >10Vpp differential swing

I. Sarkas, A. Balteanu, E. Dacquay, A. Tomkins, S. Voinigescu
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引用次数: 38

Abstract

The ever-increasing demand for low-cost portable communication devices pushes for higher integration of wireless transceivers in deeply-scaled silicon technologies. Given the overwhelming digital content of a mobile platform, ideally, the RF components should be realized with topologies that allow for their seamless scaling into 22nm and 14nm CMOS technologies. The Power Amplifier (PA) remains one of the most challenging circuit blocks to implement in nanoscale CMOS due to the strict requirements for output power, efficiency and linearity imposed by wireless communication standards. The low breakdown voltage of nanoscale MOSFETs limits the maximum drain voltage swing and the maximum achievable output power. In order to circumvent this problem, a typical approach is to increase the device size and use a reactive matching network to transform the load resistance to a value significantly lower than 50Ω. Nevertheless, due to the typically low-Q passive components that can be manufactured in a nanoscale CMOS process, and because of the high impedance transformation ratio involved, most of the additional output power that would be gained by increasing the device size is wasted in resistive losses in the matching networks, resulting in poor efficiency. This problem is exacerbated at mm-Wave frequencies where the loss of the passive components is even higher, and using lower fT/fMAX thicker oxide or extended drain MOS devices [1] is not viable.
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差分摆幅>10Vpp的45nm SOI CMOS d类毫米波PA
对低成本便携式通信设备不断增长的需求推动了无线收发器在深度硅技术中的更高集成度。考虑到移动平台中压倒性的数字内容,理想情况下,RF组件应该通过允许其无缝扩展到22nm和14nm CMOS技术的拓扑来实现。由于无线通信标准对输出功率、效率和线性度的严格要求,功率放大器(PA)仍然是纳米级CMOS中最具挑战性的电路模块之一。纳米级mosfet的低击穿电压限制了最大漏极电压摆幅和最大可实现输出功率。为了规避这个问题,一种典型的方法是增加设备尺寸,并使用无功匹配网络将负载电阻转换为显着低于50Ω的值。然而,由于典型的低q无源元件可以在纳米级CMOS工艺中制造,并且由于所涉及的高阻抗转换比,通过增加器件尺寸而获得的大部分额外输出功率都浪费在匹配网络中的电阻损失上,导致效率低下。这个问题在毫米波频率下更加严重,无源元件的损耗更高,使用更低fT/fMAX的厚氧化物或延长漏极的MOS器件[1]是不可用的。
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