Abstract:We present a four point bending setup suitable for high precision characterization of piezoresistance in semiconductors. The compact setup has a total size of 635cm3. Thermal stability is ensured by an aluminum housing wherein the actual four point bending fixture is located. The four point bending fixture is manufactured in polyetheretherketon and a dedicated silicon chip with embedded piezoresistors fits in the fixture. The fixture is actuated by a microstepper actuator and a high sensitivity force sensor me… Show more
“…The piezoresistance characterization is done in an automated four point bending fixture. This fixture applies a uniaxial, uniform stress to the resistors in the center region of the chip 33 in steps of approximately 5 to a maximum value of 70 MPa, which corresponds to a strain of ⑀ xx Ϸ 0.0004.…”
We calculate the shear piezocoefficient 44 in p-type Si with a 6 ϫ 6 k · p Hamiltonian model using the Boltzmann transport equation in the relaxation-time approximation. Furthermore, we fabricate and characterize p-type silicon piezoresistors embedded in a ͑001͒ silicon substrate. We find that the relaxation-time model needs to include all scattering mechanisms in order to obtain correct temperature and acceptor density dependencies. The k · p results are compared to results obtained using a recent tight-binding ͑TB͒ model. The magnitude of the 44 piezocoefficient obtained from the TB model is a factor of 4 lower than experimental values; however, the temperature and acceptor density dependencies of the normalized values agree with experiments. The 6 ϫ 6 Hamiltonian model shows good agreement between the absolute value of 44 and the temperature and acceptor density dependencies when compared to experiments. Finally, we present a fitting function of temperature and acceptor density to the 6 ϫ 6 model that can be used to predict the piezoresistance effect in p-type silicon.
“…The piezoresistance characterization is done in an automated four point bending fixture. This fixture applies a uniaxial, uniform stress to the resistors in the center region of the chip 33 in steps of approximately 5 to a maximum value of 70 MPa, which corresponds to a strain of ⑀ xx Ϸ 0.0004.…”
We calculate the shear piezocoefficient 44 in p-type Si with a 6 ϫ 6 k · p Hamiltonian model using the Boltzmann transport equation in the relaxation-time approximation. Furthermore, we fabricate and characterize p-type silicon piezoresistors embedded in a ͑001͒ silicon substrate. We find that the relaxation-time model needs to include all scattering mechanisms in order to obtain correct temperature and acceptor density dependencies. The k · p results are compared to results obtained using a recent tight-binding ͑TB͒ model. The magnitude of the 44 piezocoefficient obtained from the TB model is a factor of 4 lower than experimental values; however, the temperature and acceptor density dependencies of the normalized values agree with experiments. The 6 ϫ 6 Hamiltonian model shows good agreement between the absolute value of 44 and the temperature and acceptor density dependencies when compared to experiments. Finally, we present a fitting function of temperature and acceptor density to the 6 ϫ 6 model that can be used to predict the piezoresistance effect in p-type silicon.
“…In this work, four point bending (4PB) apparatus is employed to produce uniform and uniaxial stress along the <110> direction of the piezoresistors [15], [16], [21]- [23]. Figure 5 illustrates the apparatus used.…”
Section: Four Point Bending Apparatusmentioning
confidence: 99%
“…Linear bearings are employed to minimize friction as the top block moves downwards. The stress (σ) at the centre is derived as [15], [16], [21]- [23] where F is force, a is inner separation, w is width and t is the thickness of the silicon beam. Deflection is given by [15], [16], [21]- [23] where L is the length of the beam, and E is the Young's modulus of silicon.…”
Section: Four Point Bending Apparatusmentioning
confidence: 99%
“…Applying a uniaxial stress along the <110> direction, the relative resistance change for a piezoresistor can be simplified to [15], [16], [21]- [23] …”
Section: Introductionmentioning
confidence: 99%
“…The thickness and width of the chip are defined based on the dimension of the Zero Insertion Force connector (ZIF) which creates a simple plug and measure method [15], [16]. Flat flexible cable is employed to establish electrical connections to the test chip to minimize measurement error.…”
Abstract-This paper reports on the enhanced piezoresistive effect in p-type <110> silicon nanowires, fabricated using a top down approach. The silicon nanowire width is varied from 100 to 500nm with thickness of 200 nm and length of 9µm. It is found that the piezoresistive effect increases when the nanowire width is reduced below 350 nm. Compared with micrometre sized piezoresistors, silicon nanowires have produced up to 50% enhancement. Silicon nanowire with cross-section of (100 × 200 nm) with doping concentration of 3.2 × 10 18 cm -3 has produced a gauge factor of 150. The extracted gauge factors are compared with other silicon nanowire experimental publications. The enhancement in piezoresistive effect by employing non-suspended silicon nanowire is beneficial for new MEMS pressure sensors with medium doping concentrations.
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