The present invention relates to MOS (metal-oxide-semiconductor) capacitors and in particular to capacitors having variable capacitance.
MOS capacitors are one of the fundamental building blocks for integrated circuits and they are frequently used for instance in voltage controlled oscillators. A wide range of modulation is often preferred. In the voltage controlled oscillators this increases the tuning range for the oscillator.
In a MOS capacitor the maximum capacitance, which commonly is referred to as accumulation capacitance, is set by the thickness and the permittivity of the intermediate dielectric layer, while the minimum capacitance, which commonly is referred to as the depletion capacitance, is set by the doping of the semiconductor substrate, and depends on the length of the depletion region. By changing the bias for the capacitor, the capacitance can be changed between the maximum and minimum values. Conventional MOS capacitors have an inherent limitation in the capacitance modulation range and the depletion capacitance is fairly high.
In view of the foregoing one object of the present invention is to provide a MOS capacitor with a wide range of capacitance modulation and a low depletion capacitance. This is achieved by the nanostructured MOS capacitor and the method for varying a capacitance in an electric circuit by using a nanostructured MOS capacitor in accordance with the attached claims.
The nanostructured MOS capacitor according to the invention comprises a nanowire electrically connected to a first electrode, optionally a dielectric layer that covers at least a portion of the nanowire, and a gate electrode that covers at least a portion of the dielectric layer. At least a part of the nanowire and the first electrode function as the above-mentioned semiconductor body and body electrode, respectively. The gate electrode is an at least first radial layer arranged around at least a portion of the dielectric layer to form a gated portion having length L of the nanowire, and the dielectric layer is an at least second radial layer arranged around the nanowire along at least a portion of the nanowire.
In one embodiment of a nanostructured MOS capacitor in accordance with the present invention the whole nanowire cross-section of the gated portion is adapted to be completely depleted when a predetermined voltage is applied to the gate electrode.
Preferably the width of the nanowire 2 is less than 4 L, preferably less than 0.4 L, and more preferably less than 0.1 L.
Preferably the width of the nanowire 2 is less than 100 μm, preferably less than 60 μm, and more preferably less than 20 μm.
In other embodiment of the present invention the nanostructured MOS capacitor is used in an electric circuit for varying a capacitance, a voltage controlled oscillator device and a sample and hold circuit device.
Thanks to the invention it is possible to provide a MOS capacitor having an increased capacitance modulation range.
It is a further advantage of the invention to provide a MOS capacitor which has relatively low depletion capacitance compared to prior art MOS capacitances.
Embodiments of the invention are defined in the dependent claims. Other objects, advantages and novel features of the invention will become apparent from the following detailed description of the invention when considered in conjunction with the accompanying drawings and claims.
Preferred embodiments of the invention will now be described with reference to the accompanying drawings, wherein:
a-d schematically illustrate one implementation of the present invention and experimental results from C(V) measurements thereon;
The present invention is based on using a nanowire to form a nanostructured MOS capacitor.
Nariowires are usually interpreted as one dimensional nanostructures that is in nanometer dimensions in its diameter. As the term nanowire implies it is the lateral size that is on the nanoscale whereas the longitudinal size is unconstrained. Such one dimensional nanostructures are commonly also referred to as nanowhiskers, one-dimensional nano-elements, nanorods, nanotubes, etc. Generally, nanowires are considered to have at least two dimensions each of which are not greater than 300 nm. However, the nanowires can have a diameter or width of up to about 1 μm. The one dimensional nature of the nanowires provides unique physical, optical and electronic properties. These properties can for example be used to form devices utilizing quantum mechanical effects or to form heterostructures of compositionally different materials that usually cannot be combined due to large lattice mismatch. On example is integration of semiconductor materials with reduced lattice-etching constraints and allow the growth of III-V structures on many semiconductor substrates such as Si substrates. As the term nanowire implies the one dimensional nature is often associated with an elongated shape. However, nanowires can also benefit from some of the unique properties without having an elongated shape. By way of example non-elongated nanowires can be formed on a substrate material having relatively large defect density in order to provide a defect-free template for further processing or in order to form a link between the substrate material and another material. Hence the present invention is not limited to an elongated shape of the nanowires. Since nanowires may have various cross-sectional shapes the diameter is intended to refer to the effective diameter.
Referring to
The accumulation and depletion modes are determined by threshold levels for the voltage applied to the gate electrode 4. If nanowire 2 is made of a p-type material, the gated portion 7 of the nanowire 2 is adapted to be fully depleted when a voltage higher than a first predetermined threshold level is applied to the gate electrode 4. On the other hand if the nanowire 2 is made of an n-type material, the gated portion 7 of the nanowire 2 is adapted to be fully depleted when a voltage lower than a second predetermined threshold level is applied to the gate electrode 4.
The change in device area according to the present invention, when changing from accumulation mode to depletion mode, improves the modulation capability of the MOS capacitor. Basically the depletion capacitance can approach zero, which is a unique feature for the nanowire 2 geometry and not possible with conventional MOS capacitors as described with reference to
For a nanostructured MOS capacitor in accordance with one embodiment of the present invention that comprises a cylindrical nanowire 2 the capacitance, when changing capacitance-determining areas, is reduced if the width of the nanowire 2 is less than four times the length of the gated portion 7 of the nanowire 2. Preferably the width of the nanowire 2 is less than 0.4 L, and even more preferably the width of the nanowire is less than 0.1 L. A decrease of the width-to-length-ratio (W/L) gives an increased change in capacitance when changing from accumulation mode to depletion mode. To establish the complete depletion of the nanowire 2 and to provide a low depletion capacitance the width or radius of the nanowire should be small. Preferably the radius R of the nanowire 2 is less than 50 μm, preferably less than 30 μm, and more preferably less than 10 μm, i.e. the width is less than 100 μm, preferably less than 60 μm, and more preferably less than 20 μm
As understood by a skilled person, nanowires are readily processed in parallel and thus an array of nanostructured MOS capacitors can be fabricated on a common substrate. A predetermined capacitance of a nanostructured MOS capacitor device can be obtained, for example, by connecting at least a group of nanowires of an array in parallel or in series. Another possibility to vary the capacitance is to vary the dimensions, i.e. the length and the thickness of the nanowire 2, or to vary the composition or thickness of the dielectric layer.
Referring to
a-c illustrates one implementation of a nanostructured MOS capacitor of the present invention. Nanowire arrays, as in the SEM micrograph in
The dielectric layer 5 and the gate electrode 4 may enclose only a portion of the nanowire 2 or the full length thereof. In one embodiment of a nanostructured capacitor according to the invention a nanowire protrudes through a hole in an insulating growth mask 14. A dielectric layer 5 and a gate electrode 4 extend along the length of the nanowire 2 and enclose the circumferential surface thereof while leaving an end portion free for an electrical connection.
a schematically illustrates a theoretical fit of the C(V) dataset of
One embodiment of the present invention provides an electrical circuit comprising a nanostructured MOS transistor for providing a variable capacitance.
Referring to
Referring to
Referring to
The method preferably further comprises the step of 102 applying a second predetermined voltage to the gate electrode 4 to establish accumulation mode.
By varying a voltage applied to the gate electrode 4 the capacitance can be varied and in one embodiment the method comprises the steps of 103 altering between accumulation mode and depletion mode. As described above the capacitance may be defined by different capacitance-determining areas depending on whether the capacitor is operating in the depletion mode or in the accumulation mode by appropriate dimensioning of the nanostructured MOS capacitor.
While the invention has been described for single nanowires it is to be understood that a very large number (few to millions of) nanowires can be collectively used as capacitors in identical fashions.
Suitable materials for the substrate of the nanostructured MOS capacitor include, but is not limited to: Si, GaAs, GaP, GaP:Zn, GaAs, InAs, InP, GaN, Al2O3, SiC, Ge, GaSb, ZnO, InSb, SOI (silicon-on-insulator), CdS, ZnSe, CdTe. Suitable materials for the nanowires include, but is not limited to IV, III-V, II-VI semiconductors such as: GaAs, InAs, Ge, ZnO, InN, GaInN, GaN AlGaInN, BN, InP, InAsP, GaInP, InGaP:Si, InGaP:Zn, GaInAs, AlInP, GaAlInP, GaAlInAsP, GaInSb, InSb and Si. Possible donor dopants are, but not limited to, Si, Sn, Te, Se, S, etc, and acceptor dopants are Zn, Fe, Mg, Be, Cd, etc.
Although the present invention has been described in terms of nanostructured MOS capacitors, it should be appreciated that the above mentioned effect of switching between different capacitance determining areas can be utilized for other semiconductor devices such as a Schottky diode. In principle the Schottky diode functions as a MOS capacitor. A nanostructured Schottky diode according to one embodiment of the invention comprises a semiconductor nanowire 2 or an array of semiconductor nanowires protruding from a semiconductor substrate 12 or optionally a buffer layer on a semiconductor substrate 12. At least a portion of the nanowire is enclosed by a metallic contact 24 defining a gated portion 7 of the nanowire, whereby a junction between the metallic contact 24 and the semiconductor nanowire 2 forms a Schottky barrier. The metallic contact and a first electrode 21, which is connected to the nanowire via the buffer layer and/or the substrate or via a wrap contact enclosing a part of the nanowire not enclosed by the metallic contact, form a two-terminal device. The nanowire geometry enables formation of nearly defect-free materials in the device and a high packing density. In particular, wide-bandgap semiconductors such as GaN, InGaN, AlGaN, SiC, which are preferred materials for Schottky diodes, can be used. When compared to Si diodes these materials offer higher performance in terms of breakdown voltage, lower leakage currents, higher temperature stability, faster reverse recovery times and positive temperature coefficients of resistance. Suitable materials for the metallic contact are metallic materials comprising one or more of Mg, Hf, Ag, Al, W, Au, Pd or Pt. The buffer layer, which may be a III-V material comprising GaN, InN, InGaN, InP, GaAs or GaP, can be used also for the other embodiments described above.
As appreciated by the skilled person the dielectric layer 5 may comprise other materials than oxides, although the term MOS (metal-oxide-semiconductor) indicates that the dielectric material should be an oxide. The dielectric layer may be made of HfO2 as disclosed above but also other dielectric materials such as for example Al2O3, ZrO2, Si3N4 and Ga2O3 can be used.
While the invention has been described in connection with what is presently considered to be the most practical and preferred embodiments, it is to be understood that the invention is not to be limited to the disclosed embodiments, on the contrary, it is intended to cover various modifications and equivalent arrangements within the appended claims.
Number | Date | Country | Kind |
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0801393-0 | Jun 2008 | SE | national |
Filing Document | Filing Date | Country | Kind | 371c Date |
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PCT/SE2009/050734 | 6/15/2009 | WO | 00 | 12/13/2010 |