[et_pb_section fb_built=”1″ _builder_version=”3.22.3″ background_color=”#f7f7f7″ max_width_phone=”100%” max_width_last_edited=”on|desktop” custom_margin=”|||0px” custom_padding=”0px||10px” saved_tabs=”all”][et_pb_row use_custom_gutter=”on” gutter_width=”1″ custom_padding=”60px||60px|0px|true” custom_margin=”|||” custom_padding_last_edited=”on|desktop” padding_top_bottom_link_1=”true” padding_top_1=”0px” padding_bottom_1=”0px” padding_left_1=”0px” module_class=” et_pb_row_fullwidth” _builder_version=”3.22.3″ background_image=”https:\/\/www.beamtec.de\/wp-content\/uploads\/2019\/01\/End-hall-quelle-blur.jpg” width=”100%” width_tablet=”100%” width_last_edited=”on|desktop” max_width=”100%” max_width_tablet=”100%” max_width_last_edited=”on|desktop” module_alignment=”center” make_fullwidth=”on” custom_width_px=”2600px”][et_pb_column type=”4_4″ _builder_version=”3.18.4″][et_pb_blurb title=”Ion Sources” content_max_width=”718px” _builder_version=”3.19.9″ header_level=”h1″ header_font=”||||||||” header_text_align=”center” header_text_color=”#fe871f” header_font_size=”59px” header_font_size_tablet=”37px” header_font_size_phone=”25px” header_font_size_last_edited=”on|tablet” body_font=”||||||||” body_text_align=”center” body_text_color=”#ffffff” body_font_size=”30px” body_font_size_tablet=”25px” body_font_size_phone=”20px” body_font_size_last_edited=”on|phone” custom_margin=”34px||” custom_padding=”25px||25px||true” custom_padding_tablet=”0px||0px|” custom_padding_phone=”0px||0px|” custom_padding_last_edited=”on|desktop”]<\/p>\n
eH3000<\/p>\n
[\/et_pb_blurb][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=”1″ _builder_version=”3.22.3″ background_color=”#f7f7f7″ custom_padding=”0|0px|0|0px|false|false”][et_pb_row custom_padding=”0|0px|27px|0px|false|false” _builder_version=”3.22.3″][et_pb_column type=”4_4″ _builder_version=”3.19.8″][et_pb_text _builder_version=”3.22.6″]<\/p>\n
Home<\/a> \u00bb Ion Sources<\/a> \u00bb Gridless End-Hall Ion Sources<\/a> \u00bb eH3000<\/p>\n [\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=”1″ _builder_version=”3.22.3″ background_color=”#f7f7f7″ custom_padding=”0|0px|0|0px|false|false”][et_pb_row custom_padding=”27px|0px|0|0px|false|false” _builder_version=”3.22.3″][et_pb_column type=”3_5″ _builder_version=”3.19.9″][et_pb_text _builder_version=”3.19.9″ text_font=”||||||||” text_orientation=”justified”]<\/p>\n The eH3000 is the largest and most powerful of the eH products. Its size and output make it best suited for high power applications and high throughput production systems. The eH3000 outputs the high current density needed to ion assist film growth in large coating plants. For example, installation in deposition systems with critical dimensions greater than 1meter, it achieves favorable film properties in packing density, stress, environmental stability and stoichiometry. Compared to other high power plasma sources, the eH3000 excels at return on investment and is the most efficient and high ion flux plasma source available.<\/p>\n [\/et_pb_text][et_pb_image src=”https:\/\/www.beamtec.de\/wp-content\/uploads\/2019\/01\/EH3000-plasma.jpg” align=”center” _builder_version=”3.19.9″ max_width=”40%”][\/et_pb_image][\/et_pb_column][et_pb_column type=”2_5″ _builder_version=”3.19.9″][et_pb_text _builder_version=”3.19.9″ text_font=”||||||||” ol_font=”||||||||” header_font=”||||||||” module_alignment=”center” animation_style=”slide” animation_delay=”200ms” animation_intensity_slide=”0%”]<\/p>\nSpecifications<\/h2>\n
| Discharge power<\/td>\n | 3000 W max<\/td>\n<\/tr>\n |
| Anode current<\/td>\n | 20 A<\/td>\n<\/tr>\n |
| Beam current<\/td>\n | 2000 mA max<\/td>\n<\/tr>\n |
| Anode voltage<\/td>\n | 250 V max<\/td>\n<\/tr>\n |
| Mean beam energy<\/td>\n | 35 – 200 eV<\/td>\n<\/tr>\n |
| Gas flow<\/td>\n | 1 – 150 sccm<\/td>\n<\/tr>\n |
| Divergence<\/td>\n | 60\u00b0<\/td>\n<\/tr>\n |
| Operating pressure<\/td>\n | up to 1 x 10-3 mbar<\/td>\n<\/tr>\n |
| Height<\/td>\n | 150 mm<\/td>\n<\/tr>\n |
| Weight<\/td>\n | 3,6 kg<\/td>\n<\/tr>\n<\/tbody>\n<\/table>\n <\/p>\n [\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=”1″ _builder_version=”3.22.3″ background_color=”#f7f7f7″ custom_padding=”0|0px|54px|0px|false|false”][et_pb_row _builder_version=”3.22.3″][et_pb_column type=”2_5″ _builder_version=”3.19.9″][et_pb_image src=”https:\/\/www.beamtec.de\/wp-content\/uploads\/2019\/01\/EH3000WCA.png” _builder_version=”3.19.9″ max_width=”35%” max_width_tablet=”30%” max_width_last_edited=”on|phone” module_alignment=”center”][\/et_pb_image][\/et_pb_column][et_pb_column type=”3_5″ _builder_version=”3.19.9″][et_pb_text _builder_version=”3.19.9″]<\/p>\n Die eH3000 can be used with a filament as well as a hollow cathode for the neutralization and plasma discharge. [\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=”1″ _builder_version=”3.22.3″ background_color=”#f7f7f7″][et_pb_row _builder_version=”3.22.3″][et_pb_column type=”4_4″ _builder_version=”3.19.8″][et_pb_toggle title=”Features & Benefits” _builder_version=”3.19.17″ title_level=”h2″ title_font=”||||||||” title_text_color=”#fe871f”]<\/p>\n Divergent Beam<\/h3>\nFrom the plasma discharge, ions accelerate into a beam with a divergent ion current flux. The half maximum-half angle exceeds a 45\u00ba angle from the source axis. The divergent beam from an eH product covers a large area. The capability to uniformly cover a wide process zone facilitates high throughput operation, since a process run with a large load of parts or large substrate area becomes practical with an eH product.<\/p>\n Gridless<\/h3>\nThe eH product technology relies on a gridless construction. The ions accelerate directly from the plasma discharge to form the beam. The gridless eH technology complements our gridded ion source products, because it produces desirable beam properties not easily available with gridded sources. Other benefits of the eH gridless feature, include no need to maintain, align or replace grids. The eH products are rugged and simple to operate. And they typically cost less than their gridded counterparts.<\/p>\n High Density DC Discharge<\/h3>\nThe sources utilize a well-proven and efficient plasma generation process. In the discharge chamber, a cathode thermionically emits a reliable source of electrons. The electrons are attracted to a DC biased metal anode. The neutral gas species is efficiently ionized due to a confining magnetic field. This mechanism produces a high density plasma of many gases, including Ar, Xe, O2, N2 and other reactive gases.<\/p>\n Low Energy & High Current Output<\/h3>\nThe eH products output a high current and low energy beam. The high ion current meets critical arrival ratios for high process rates. Also, the high current enables productive processing on tough, hard materials. While the low energy ion bombardment eliminates damage to surfaces and interfaces. The capability to process at low energies has proven merit when working with delicate materials.<\/p>\n Non-immersed neutralizers<\/h3>\nThe standard neutralizer configuration is an inexpensive refractory metal filament stretched across the ion beam. The filament is heated to thermionic emission temperature. The filament neutralizer may be replaced with an alternative non-immersed neutralizer. The non-immersed neutralizer sits to the side of the source and outside the ion beam. When the neutralizer is outside the beam, the time between maintenance is significantly longer for the non-immersed neutralizer versus the filament neutralizer. This non-immersed configuration is suited for low frequency maintenance installations and long operational runs when it is important to minimize the risk of process interruption.<\/p>\n Quick Change Anode Module<\/h3>\nThe eH Product incorporates our patented quick- change anode module assembly. The anode module can be quickly removed from the ion source for maintenance, while the source body remains in the chamber. The anode module is light weight and interchangeable. By simply exchanging the working anode module with a spare module, the eH product can be ready to run within minutes. The removed anode module can be easily maintained on a work bench while your vacuum chamber continues to be productive. The uptime benefits are significant.<\/p>\n Stable Neutralization<\/h3>\nThe product line provides a dedicated and regulated electron source neutralizer. With a reliable source of electrons, the products can process dielectric, electrically isolated, and electrostatic sensitive substrates. The amount of electrons is precisely controlled to match positive charges. The correct amount electrons are present in the ion beam and they arrive at the substrate surface to provide an electrically neutral process. The operation does not need to rely on an ambiguous source of electrons such as exposed and conductive chamber hardware. Coating build-up and stray electromagnetic fields, which may be present in the vacuum chamber, will not disturb the ion beam quality, stability or neutralization of the products. However, in the case, when the neutralization process is not so critical, the products do allow operation without the neutralizer.<\/p>\n [\/et_pb_toggle][\/et_pb_column][\/et_pb_row][\/et_pb_section]<\/p>\n","protected":false},"excerpt":{"rendered":" eH3000Home \u00bb Ion Sources \u00bb Gridless End-Hall Ion Sources \u00bb eH3000 The eH3000 is the largest and most powerful of the eH products. Its size and output make it best suited for high power applications and high throughput production systems. The eH3000 outputs the high current density needed to ion assist film growth in large […]<\/p>\n","protected":false},"author":2,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_et_pb_use_builder":"on","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"class_list":["post-4374","page","type-page","status-publish","hentry"],"yoast_head":"\n |