Measurements of an ion beam diameter extracted into air through a large-bore metal capillary

Author(s):  
Y. Hirano ◽  
M. Umigishi ◽  
K. Ishii ◽  
H. Ogawa
Author(s):  
Valery Ray ◽  
Josef V. Oboňa ◽  
Sharang Sharang ◽  
Lolita Rotkina ◽  
Eddie Chang ◽  
...  

Abstract Despite commercial availability of a number of gas-enhanced chemical etches for faster removal of the material, there is still lack of understanding about how to take into account ion implantation and the structural damage by the primary ion beam during focused ion beam gas-assisted etching (FIB GAE). This paper describes the attempt to apply simplified beam reconstruction technique to characterize FIB GAE within single beam width and to evaluate the parameters critical for editing features with the dimensions close to the effective ion beam diameter. The approach is based on reverse-simulation methodology of ion beam current profile reconstruction. Enhancement of silicon dioxide etching with xenon difluoride precursor in xenon FIB with inductively coupled plasma ion source appears to be high and relatively uniform over the cross-section of the xenon beam, making xenon FIB potentially suitable platform for selective removal of materials in circuit edit application.


Author(s):  
Xiang-Wen Xiong ◽  
Bear L. Wynn

The method of electronic parallel datum is to calculate by a stereo angle between the two beams of light with inclination simulating parameters of an object and successfully replace the 6-DOF mechanical datum of the work piece by being pre-set in the work piece and system. This technique called electronic parallel datum method has high precision for the adoption of Scan & Micro-Staggered method; furthermore, the intelligent direct reading of 6-DOF mechanical datum and parameter storage function of the technique can greatly improve the performance of the system and at the same time offer the process control method and can be used for micro-fabrication and Micro-Manufacturing and general industrial (In particular, it can be used for Ultra precision manufacturing environment, because the diameter of the laser beam can reach 100 nm and ion beam diameter even reached the limit precision of 2nm, and optical emission types, including the ion beam, Universal laser beam and general light beam, which mainly use receiver spacing of nano-array CCD sensors). It is widely used in the intelligent control process and system such as installation and adjustment, and undoubtedly, is to be adopted in many technical fields, general Manufacturing and all general work piece, precise testing process. With the method the system will become more precise, run faster and cost less.


Author(s):  
Steven J. Pachuta

Time-of-flight secondary ion mass spectrometry (TOF-SIMS) has in recent years become a useful tool for surface analysis in industrial laboratories. All elements and isotopes, as well as many molecular entities, can be detected by SIMS, with most of the signal coming from the outer 10 - 20 Å of the surface. The initial penetration of TOF-SIMS into industry was as an improvement over existing quadrupole instruments, with higher mass range, mass resolution, and sensitivity. The coupling of TOF-SIMS with high brightness liquid metal ion sources greatly expanded the applicability of the technique, making chemical imaging of the outermost monolayers of a surface a routine experiment.Several examples will be presented of TOF-SIMS imaging applied to real-world materials encountered in an industrial analytical laboratory. All results were obtained from a PHI-Evans TFS series instrument equipped with an FEI two-lens 69Ga+ liquid metal ion gun (LMIG). When operated at 25 keV beam energy, a primary ion beam diameter of 2500 Å in continuous mode, and 1-2 μm in pulsed mode, can routinely be obtained.


2001 ◽  
Vol 65 (2) ◽  
pp. 107-129 ◽  
Author(s):  
STEINAR BØRVE ◽  
HANS L. PÉCSELI ◽  
JAN TRULSEN

The formation and propagation of ion phase-space vortices are observed in a numerical particle-in-cell simulation in two spatial dimensions and with three velocity components. The code allows for an externally applied magnetic field. The electrons are assumed to be isothermally Boltzmann-distributed at all times, implying that Poisson's equation becomes nonlinear for the present problem. Ion phase-space vortices are formed by the nonlinear saturation of the ion-ion two-stream instability, excited by injecting an ion beam at the plasma boundary. We consider the effect of a finite beam diameter and a magnetic field, in particular. A vortex instability is observed, appearing as a transverse modulation, which slowly increases with time and ultimately breaks up the vortex. When many vortices are present at the same time, we find that it is their interaction that eventually leads to a gradual filling-up of the phase-space structures. The ion phase-space vortices have a finite lifetime, which is noticeably shorter than that found in one-dimensional simulations. An externally imposed magnetic field can increase this lifetime considerably. For high injected beam velocities in magnetized plasmas, we observe the excitation of electrostatic ion-cyclotron instabilities, but see no associated formation of ion phase-space vortices. The results are relevant, for instance, for the interpretation of observations by instrumented spacecraft in the Earth's ionosphere and magnetosphere.


1989 ◽  
Vol 147 ◽  
Author(s):  
John Melngailis ◽  
Patricia G. Blauner

AbstractFocused ion beam induced deposition is already in use commercially for the repair of clear defects in photomasks, where missing absorber is added. Research is being carried out to extend this technique to the repair of x-ray lithography masks and to the restructuring and repair of integrated circuits, particularly in the prototype phase. In this technique a local gas ambient is created, for example, by aiming a small nozzle at the surface. The gas molecules are thought to adsorb on the surface and to be broken up by the scanned focused ion beam. A deposit is formed with linewidth equal to the beam diameter which can be below 0.1 Ό m. At small beam diameters and low currents (50–100 pA) the time to deposit 1Όm3 is in the vicinity of 10–20 sec. If the gas is a hydrocarbon, the deposit is largely carbon, which is useful for photomask repair. On the other hand, if the gas is a metal halide or a metal organic, the deposit is metallic. The deposits have substantial concentrations of impurities due to the atoms in the organometallic, to the ion species used, or to the ambient in the vacuum chamber. Thus the resistivities of the "metal" films deposited typically range from 150 to 1000 ΌΏcm which is usable for some repairs. (Pure metals have resistivities in the range 2.5 to 12 pQcm.) We have deposited gold from dimethyl gold hexafluoro acetylacetonate and have achieved linewidths down to 0.1 Όm, patches of 1 Όm thickness with steep side walls and in some cases, resistivities approaching the bulk value. Other workers have reported deposits of Al, W, Ta, and Cr. We will review previous work in the field and present some of our own current results.


2003 ◽  
Vol 792 ◽  
Author(s):  
H. Wanzenboeck ◽  
S. Harasek ◽  
H. Langfischer ◽  
B. Basnar ◽  
W. Brezna ◽  
...  

ABSTRACTThe focused ion beam has been acknowledged as a versatile tool for local sputtering as well as local deposition of material. A beam diameter below 10 nm is feasible and renders FIB a powerful tool for microstructure fabrication and generation. This experimental study investigates the geometrical limitations of FIB processing as well as the implications on the processed material. The high energetic ions of the primary beam also change the properties of the processed material due to implantation and atomic mixing. The incorporation of Ga from the FIB may be beneficial in the case of deliberate implantation or unfavorable as a chemical impurity. Higher doses of ion irradiation caused amorphisation of the material. The effects of FIB processing on the substrates as well as deposited structures are illustrated.


2014 ◽  
Vol 20 (5) ◽  
pp. 1514-1520 ◽  
Author(s):  
Radovan Urban ◽  
Robert A. Wolkow ◽  
Jason L. Pitters

AbstractIn this paper we investigate methods to characterize angular current density from atomically defined gas field ion sources. We show that the ion beam emitted from a single apex atom is described by a two-dimensional Gaussian profile. Owing to the Gaussian shape of the beam and the requirement to collect the majority of the ion current, fixed apertures have inhomogeneous illumination. Therefore, angular current density measurements through a fixed aperture record averaged angular current density. This makes comparison of data difficult as averaged angular current density depends on aperture size. For the same reasons, voltage normalization cannot be performed for fixed aperture measurements except for aperture sizes that are infinitely small. Consistent determination of angular current density and voltage normalization, however, can be achieved if the beam diameter as well as total ion current are known. In cases where beam profile cannot be directly imaged with a field ion microscope, the beam profile could be extracted from measurements taken at multiple acceleration voltages and/or with multiple aperture sizes.


1990 ◽  
Vol 181 ◽  
Author(s):  
Khanh Q. Tran ◽  
Yuuichi Madokoro ◽  
Tohru Ishitani ◽  
Cary Y. Yang

ABSTRACT30-keV focused Ga+ ion beam was used for induced deposition of small-area tungsten thin films from W(CO)6 on Si and SiO2. Deposition yield, calculated assuming pure tungsten depositions, depends on dwell time (beam diameter/scan speed) and beam current density. High current density and/or long dwell time are known to cause low deposition yield because of the depletion of adsorbed gas molecules during ion beam irradiation. Based on a model taking this effect into account, numerical fitting was carried out. The reaction cross-section was estimated to be 1.4 × 10−14 cm2. For doses below 1017 ions/cm2, film resistivity decreases with increasing dose. This was confirmed for several dwell times. However, for doses above 1017 ions/cm2, film resistivity remains independent of dose. In this “high”-dose range, variation of beam current density has little effect on film resistivity. AES analyses revealed a consistency between film composition and resistivity. For a “high”-dose film with a resistivity of 190 μΩ-cm, the approximate tungsten content was 50 at%.


2001 ◽  
Vol 7 (S2) ◽  
pp. 796-797
Author(s):  
Lucille A. Giannuzzi

In a focused ion beam (FIB) instrument, ions (typically Ga+) obtained from a liquid metal ion source are accelerated down a column at energies up to ∽ 50 keV. The beam of ions is focused by electrostatic and octopole lens systems and the ion dose (and beam diameter) is controlled using real and/or virtual apertures. Beam sizes in FIB instruments on the order of 5-7 nm may be achieved.The versatility of the FIB instrument enables large regions of material (e.g., 500 μm3) to be removed at high beam currents in just a couple of minutes. Lower beam currents (i.e., beam diameters) are usually used to remove smaller amounts of material within the same time frame (e.g., ∽ 5μm3). The introduction of an organometallic gas in close proximity to the target allows for the deposition of metals, SiO2, and other materials, by an ion beam assisted chemical vapor deposition process.


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