sputter

1 the noise of something spattering or sputtering explosively; "he heard a spatter of gunfire" [syn: spatter, spattering, splatter, splattering, splutter, sputtering]

2 an utterance (of words) with spitting sounds (as in rage) [syn: splutter]

1 make an explosive sound; "sputtering engines"

2 cause to undergo a process in which atoms are removed; "The solar wind protons must sputter away the surface atoms of the dust"

3 climb awkwardly, as if by scrambling [syn: clamber, scramble, shin, shinny, skin, struggle]

4 utter with a spitting sound, as if in a rage [syn: splutter]

5 spit up in an explosive manner [syn: splutter, spit out]

English

Etymology

From the root of spout or spit to eject from the mouth.

Pronunciation

• Rhymes: -ʌtə(r)

Noun

1. Moist matter thrown out in small detached particles; also, confused and hasty speech.

Verb

1. To spit, or to emit saliva from the mouth in small, scattered portions, as in rapid speaking.
2. To utter words hastily and indistinctly; to speak so rapidly as to emit saliva.

   They could neither of them speak their rage, and so fell a sputtering at one another, like two roasting apples. -Congreve.

3. To throw out anything, as little jets of steam, with a noise like that made by one sputtering.

   Like the green wood...sputtering in the flame. -Dryden.

4. To spit out hastily by quick, successive efforts, with a spluttering sound; to utter hastily and confusedly, without control over the organs of speech.

   In the midst of caresses, and without the last pretend incitement, to sputter out the basest accusations. -Swift.

5. To cause surface atoms or electrons of a solid to be ejected by bombarding it with heavy atoms or ions
6. To coat the surface of an object by sputtering

References

Sputtering is a process whereby atoms are ejected from a solid target material due to bombardment of the target by energetic ions. It is commonly used for thin-film deposition, etching and analytical techniques (see below).

Physics of sputtering

Physical sputtering is driven by momentum exchange between the ions and atoms in the material, due to collisions. The incident ions set off collision cascades in the target. When such cascades recoil and reach the target surface with an energy above the surface binding energy, an atom can be ejected. If the target is thin on an atomic scale the collision cascade can reach the back side of the target and atoms can escape the surface binding energy `in transmission'. The average number of atoms ejected from the target per incident ion is called the sputter yield and depends on the ion incident angle, the energy of the ion, the masses of the ion and target atoms, and the surface binding energy of atoms in the target. For a crystalline target the orientation of the crystal axes with respect to the target surface is relevant.

The primary particles for the sputtering process can be supplied in a number of ways, for example by a plasma, an ion source, an accelerator or by a radioactive material emitting alpha particles.

A model for describing sputtering in the cascade regime for amorphous flat targets is Thompson's analytical model . An algorithm that simulates sputtering based on a quantum mechanical treatment including electrons stripping at high energy is implemented in the program TRIM (www.srim.org) described in "Stopping and Range of Ions in Solids."

A different mechanism of physical sputtering is heat spike sputtering. This may occur when the solid is dense enough, and the incoming ion heavy enough, that the collisions occur very close to each other. Then the binary collision approximation is no longer valid, but rather the collisional process should be understood as a many-body process. The dense collisions induce a heat spike (= thermal spike), which essentially melts the crystal locally. If the molten zone is close enough to a surface, large amounts of atoms may sputter due to flow of liquid to the surface and/or microexplosions. Heat spike sputtering is most important for heavy ions (say Xe or Au or cluster ions) with energies in the keV–MeV range bombarding dense but soft metals with a low melting point (Ag, Au, Pb, ...). The heat spike sputtering often increases nonlinearly with energy, and can for small cluster ions lead to dramatic sputtering yields per cluster of the order of 10000 .

Physical sputtering has a well-defined minimum energy threshold which is equal to or larger than the ion energy at which the maximum energy transfer of the ion to a sample atom equals the binding energy of a surface atom. This threshold typically is somewhere in the range 10–100 eV.

Preferential sputtering can occur at the start when a multicomponent solid target is bombarded and there is no solid state diffusion. If the energy transfer is more efficient to one of the target components, and/or it is less strongly bound to the solid, it will sputter more efficiently than the other. If in an AB alloy the component A is sputtered preferentially, the surface of the solid will, during prolonged bombardment, become enriched in the B component thereby increasing the probability that B is sputtered such that the composition of the sputtered material will be AB.

Electronic sputtering

The term electronic sputtering can mean either sputtering induced by energetic electrons (for example in a transmission electron microscope), or sputtering due to very high-energy or highly charged heavy ions which lose energy to the solid mostly by electronic stopping power, where the electronic excitations cause sputtering.

Potential sputtering

In the case of multiply charged projectile ions a particular form of electronic sputtering can take place which has been termed potential sputtering. In these cases the potential energy stored in multiply charged ions (i.e., the energy necessary to produce an ion of this charge state from its neutral atom) is liberated when the ions recombine during impact on a solid surface (formation of hollow atoms). This sputtering process is characterized by a strong dependence of the observed sputtering yields on the charge state of the impinging ion and can already take place at ion impact energies well below the physical sputtering threshold . Potential sputtering has only been observed for certain target species and requires a minimum potential energy .

Applications and phenomena

Film deposition

main Sputter deposition

Sputter deposition is a method of depositing thin films by sputtering, i.e. eroding, material from a "target," e.g., SiO2, which then deposits onto a "substrate," e.g., a silicon wafer. Resputtering, in contrast, involves re-emission of the deposited material, e.g., SiO2, during the deposition also by ion bombardment.

Sputtered atoms ejected into the gas phase are not in their thermodynamic equilibrium state, and tend to deposit on all surfaces in the vacuum chamber. A substrate (such as a wafer) placed in the chamber will be coated with a thin film. Sputtering usually uses an argon plasma.

Etching

Removing atoms by sputtering with an inert gas is called `ion milling' or 'ion etching'.

Sputtering can also play a role in reactive ion etching (RIE), a plasma process carried out with chemically active ions and radicals, for which the sputtering yield may be enhanced significantly compared to pure physical sputtering. Reactive ions are frequently used in SIMS equipment to enhance the sputter rates. The mechanisms causing the sputtering enhancement are not always well understood, but for instance the case of fluorina etching of Si has been modelled well theoretically.

Sputtering which is observed to occur below the threshold energy of physical sputtering, is also often called chemical sputtering. The mechanisms behind such sputtering are not always well understood, and may be hard to distinguish from chemical etching. At elevated temperature chemical sputtering of carbon can be understood to be due to the incoming ions weakening bonds in the sample, which then desorb by thermal activation . The hydrogen-induced sputtering of carbon-based materials observed at low temperatures has been explained by H ions entering between C-C bonds and thus breaking them, a mechanism dubbed swift chemical sputtering.

For analysis

Another application of sputtering is to etch away the target material. One such example occurs in Secondary Ion Mass Spectroscopy (SIMS), where the target sample is sputtered at a constant rate. As the target is sputtered, the concentration and identity of sputtered atoms are measured using Mass Spectroscopy. In this way the composition of the target material can be determined and even extremely low concentrations (20 µg/kg) of impurities detected. Furthermore, because the sputtering continually etches deeper into the sample, concentration profiles as a function of depth can be measured.

In space

Sputtering is one of the forms of space weathering, a process that changes the physical and chemical properties of airless bodies, such as asteroids and our moon. It is also one of the possible ways that Mars has lost its atmosphere.

External links

• What is Sputtering? - an introduction with animations
• Free particle simulation program capable of modeling sputtering
• American Vacuum Society short courses on thin film deposition
• Reactive Sputtering Using A Dual-Anode Magnetron System
• Sputtering Technical and Safety Data
• sputtering target list
• picture of sputtering target

References

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