Method of forming silicon structures with selectable optical characteristics

Abstract

Silicon and metal are coevaporated onto a silicon substrate in a molecular beam epitaxy system with a larger than stoichiometric amount of silicon so as to epitaxially grow particles of metal silicide embedded in a matrix of single crystal epitaxially grown silicon. The particles interact with incident photons by resonant optical absorption at the surface plasmon resonance frequency. Controlling the substrate temperature and deposition rate and time allows the aspect ratio of the particles to be tailored to desired wavelength photons and polarizations. The plasmon energy may decay as excited charge carriers or phonons, either of which can be monitored to indicate the amount of incident radiation at the selected frequency and polarization.

Description

SUMMARY OF THE INVENTION

Briefly, the instant invention contemplates adjusting the silicide particle growth parameters so as to generate particles having specific shapes and orientations. The most important shape parameter is the aspect ratio: the ratio of the elongated dimension of the particle to the perpendicular shorter dimension. By choosing the shape and orientation of the silicide particles, the matrix of particles can be tailored to interact better with specific wavelengths of light.

For example, if the light is received perpendicular to the plane of the substrate, so that the electric field is parallel to the substrate, and the column like particles are grown to be perpendicular to the substrate as well, then taller or thinner particles ( those with higher aspect ratios) are more responsive to shorter wavelengths. Lower aspect ratio particles having either greater diameters, shorter lengths, or both, are more responsive to longer wavelengths.

However, if the particles are oriented more parallel to the substrate, so as to be more parallel to the electric field of the incident light, higher aspect ratio particles will respond more to longer wavelengths. This is because when the electric field of the light is aligned with the longer dimension of the silicide particles, longer wavelength resonance is experienced.

The ability to selectively interact with photons allows many new silicon based optical devices to be constructed. Silicon is a desirable material because integrated circuitry can be fabricated with the optical matrix components. Also, silicon has attractive mechanical and thermal properties. Examples of devices that could use wavelength specific optical layers include optical computing elements, holographic devices, optical correlators, optical phase conjugators, bistable memory devices, optical limiters, polarization filters, and infrared and visible light detectors. Two kinds of light detectors are described hereinafter that utilize optical components constructed according to the principles of the present invention. But the utility of the invention is not limited just to detectors.

The transfer of energy from the photon to the silicide particle takes place by surface plasmon resonance. Afterwards, the plasmon can decay into the excitation of a single charge carrier, a hole or an electron, so as to be electronically detectable as a current change in the silicon matrix surrounding the silicide particles. Alternatively, the plasmon may decay by mechanisms that heat the silicon matrix. This heat can be measured to detect the capture of the photon. With either readout, an efficient optical detector may be built that can be optimized for a particular wavelength of light and tailored to the linear and non-linear optical properties that may be encountered in the detector structure. Additional benefits and advantages are explained in the following detailed description and the drawings referenced thereby.

BRIEF DESCRIPTION OF THE DRAWING

FIG. 1 schematically shows the molecular beam epitaxy process used to form the optically tailored silicide particles.

FIG. 2 is a schematic diagram of the layers of an optical detector assembled in accordance with the principles of this invention.

FIG. 3 is a graph showing the shift in the peak absorption wavelength for various aspect ratio particles.

FIG. 4 shows another embodiment of the invention using different orientation particles.

FIG. 5 shows a way to measure current created in an optical detector from absorbed photons.

FIG. 6 shows a way to measure heat created in a detector by absorbed photons.

DETAILED DESCRIPTION OF THE INVENTION

FIG. 1 demonstrates the basic process used to create the silicide particle shapes that respond to selected wavelength photons. A silicon substrate 10 is processed in a high vacuum MBE system chamber. Substrate 10 is cleaned by standard techniques well known to those skilled in the art so as to produce an atomically clean surface 12. Substrate 10 is heated to a temperature such that arriving atoms of the deposition material have an interval of movement on surface 12 sufficient to locate the desired bonding sites. For the metal silicides, temperatures in the range of 640 to 800 degrees centigrade have been successfully used. In this specification, the deposited material is cobalt disilicide. But other metal silicides such as chromium disilicide may be used.

For cobalt disilicide columnar particles, cobalt and silicon are coevaporated in the MBE chamber and directed onto surface 12. The ratio of cobalt to silicon is intentionally made non-stoichiometric with an excess of silicon. This silicon rich deposition produces the particles. The cobalt atoms, being temporarily mobile on surface 12, seek out and coalesce with other cobalt disilicide molecules at random locations, establishing growth centers upon which columns 14 of single crystal cobalt silicide grow. The excess silicon forms a single crystal matrix 16, between and around columns 14, depicted as a transparent matrix 16 with dashed lines 16. The shape and locations of the columns are selectable. By raising the substrate temperature or decreasing the rate of deposition, the interval of mobility on surface 12 is lengthened so that columns are produced which are farther apart and have larger diameters. Alternatively, the ratio of silicon to metal may be changed. Less metal results in columns of the same spacing but lesser diameter. Shuttering the cobalt beam stops column growth when desired. New columns can then be initiated by unblocking the cobalt beam.

FIG. 2 shows a small portion of an optical detector 40 constructed using the process of FIG. 1. Substrate 10 is coated with the matrix 16 with the embedded cobalt disilicide particles 14, as in FIG. 1. The cobalt is shuttered to deposit a layer of intrinsic silicon 18, perhaps 40 nanometers thick, followed by two more matrix layers of silicide particles in silicon 20 separated by two layers of intrinsic silicon 22. Any number of alternating layers may be used, but a detector with three or four matrix layers of particles has been found to be efficient in the preferred embodiment.

Particles 14 typically have aspect ratios in the range of about one to ten. Each particle may comprise perhaps a thousand to a million atoms and are, thus, very small. They are, in fact, much smaller than the wavelength of the light being detected. This scale of microstructure requires analysis by effective medium theory which tells one how to calculate the effective dielectric constant for a composite material composed of different crystal structures. Each particle can be thought of as containing a sea of electrons, a plasma of sorts, that interacts with incident photons as a group.

The interaction can happen only in quantized units known as plasmons. The interaction is more probable for photons of a frequency corresponding to the surface plasmon resonance frequency of the silicide particles 14. This resonance frequency depends on the orientation of the particles relative to the electric field of the incident light and the shape of particles 14.

FIG. 3 graphs the absorption of photons relative to their energy for four different aspect ratio particles. Four curves A, B, C, and D are shown corresponding respectively to substrate temperatures, during column deposition, of 650, 700, 750, and 800 degrees Centigrade. The progressively higher temperatures produce progressively greater diameter, and thus lower aspect ratio, particles. It can be seen that the absorption peaks, P.sub.1 through P.sub.4, occur at ever lower energies, associated with longer wavelength photons, for lower aspect ratio particle shape. The graph of FIG. 3 applies to the detector of FIG. 2 where light is received perpendicular to the substrate 10, as shown by arrow 24, so that the electric field of the light is perpendicular to the long dimension of particles 14. If the orientation of the elongated particles is changed relative to the electric field, the effect is reversed. An altered orientation design is shown in FIG. 4.

In FIG. 4, several layers of particle filled matrix 26 are deposited between layers of intrinsic silicon 28. However, the particles 30 are grown as horizontally elongated structures, parallel to the electric field of incident photons 32. In this orientation, higher aspect ratio particles will have their peak absorptions shifted toward longer wavelengths.

To create the horizontal particles 30 of FIG. 4, conventional electron beam lithography methods may be used to form horizontally elongated cobalt disilicide deposits with the desired shape and position. Electron beam lithography has the advantage that the particles can be made more identical to each other and in more regular and periodic arrays. This allows a higher degree of tunability, but is more expensive. Alternatively, the horizontal particle shapes can be obtained without the cost of lithographic methods by choosing a wafer that is cut in a different plane to produce a different substrate surface for particle growth. For example, a (110) oriented wafer encourages elongated particles to form parallel to the surface.

The particle shape can be chosen to favor not only specific wavelengths, but also specific polarizations of light. If the incident light 32 is first filtered through a polarization filter, it will still be parallel to the surface of the detector, but only in a single direction. Thus, the direction of the elongate axis of particles 30 determines their effective aspect ratio relative to the incident light. Rotation of the detector, therefore, shifts the absorption peak, allowing the selection of different color light.

Once the energy of the photon has been transferred to the particle, it may be used to create charge carriers in the silicon matrix, thus, affecting the current flow through the optical detector 40 as shown in FIG. 5. The current can be sensed by a sensor 42, connected to detector 40 through a layer of P type material and a layer of N type material, as a measure of the amount of incident radiation.

Alternatively, the photon added energy in the particles can be dissipated as heat energy in the lattice vibrations of the crystalline structure as shown in FIG. 6. FIG. 6 comprises a schematic diagram of a Golay cell type optical detector. A particle filled matrix of silicon 50 is etched to form a cavity 52 and a membrane 56. Cavity 52 is closed by another layer of silicon 54 bonded to silicon matrix 50. Cavity 52 may be filled with a gas such as xenon. Incident light interacts with the particles in matrix 50, thus, heating it. The heat is conducted into the gas in cavity 52, causing the gas to expand and push membrane 56 upward in FIG. 6. Movement of the silicon membrane 56 can be sensed by an expansion detector 58 through a suitable connection 60. One such detector 58 could comprise a tunnel current probe positioned very close to the surface of the membrane 56 to measure changes in tunnel current therefrom. Such measurements are well known to those skilled in the art of scanning tunneling microscopes.

In the case of a charge carrier producing optical detector, at least one semiconductor layer, such as layer 18 in FIG. 2, must be added to gather the charge carriers before they are thermalized. However, a plurality of layers, as shown in FIG. 2, produces a more efficient detector 40.

Many variations to the present invention are possible. The above discussion is specific to silicon, which is attractive for its ease of integration with CCD or MOSFET circuitry, and also for the fact that the highest quality epitaxial growth of a metal on a semiconductor has been achieved with cobalt disilicide on silicon. However, other metal silicides using platinum, nickel, or palladium may be used. The metal silicides may be used semiconducting. Other matrix materials are a possibility as well. Germanium with germanide particles or compound semiconductors with metal particles comprise other possible systems.

Although optical detectors have been described in greater detail, the inventive optical components using specially shaped particles at selected orientations are useful in filters, memories, optical computer devices, and other optical devices tailored to respond in a linear or non-linear fashion to incident radiation of selected wavelengths. Hence, we intend limitation only in accordance with the appended claims and their equivalents.

Claims

1. A method of making an optical component with a selectable optical response comprising the steps of:

holding a semiconductor substrate in a vacuum at an elevated temperature sufficient to allow molecular mobility thereon;

directing molecular beams of metal and semiconductor material at said substrate, for a selected time, and in proportions that include an excess of semiconductor material so as to form on said substrate an epitaxial growth of semiconductor single crystal matrix with particles of single crystal metal and semiconductor compounds embedded in said matrix; and

controlling said elevated temperature and said selected time so as to achieve a predetermined aspect ratio for said particles to obtain desired optical response characteristics.

2. The method of claim 1 in which said substrate is silicon and said molecular beam of semiconductor material comprises silicon.

3. The method of claim 2 in which said metal is cobalt.

4. The method of claim 1 including the step of depositing at least one layer of intrinsic semiconductors on top of said matrix (so as to gather) whereby the gathering of charge carriers from said matrix is facilitated when said optical component is used as a detector of optical radiation.

5. The method of claim 4 including depositing additional matrix layers and intrinsic semiconductor layers.