No | Relevant item(s) from Annex to Regulation (EC) No 1183/2007 | Description |
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I.3A.001 | ex 3A001.a* | Electronic components, as follows:
a. General purpose integrated circuits, as follows:
Note 1: The prohibition status of wafers (finished or unfinished), in which the function has been determined, is to be evaluated against the parameters of I.3A.001.a.
Note 2: Integrated circuits include the following types:
‘ Monolithic integrated circuits ’ ;
‘ Hybrid integrated circuits ’ ;
‘ Multichip integrated circuits ’ ;
‘ Film type integrated circuits ’ , including silicon-on-sapphire integrated circuits;
‘ Optical integrated circuits ’ .
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I.3A.002 | 3A101 | Electronic equipment, devices and components, as follows:
a. Analogue-to-digital converters, usable in ‘ missiles ’ , designed to meet military specifications for ruggedized equipment;
b. Accelerators capable of delivering electromagnetic radiation produced by bremsstrahlung from accelerated electrons of 2 MeV or greater, and systems containing those accelerators.
Note: I.3A.002.b. above does not specify equipment specially designed for medical purposes.
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I.3A.003 | 3A201 | Electronic components as follows;
a. Capacitors having either of the following sets of characteristics:
1. a. Voltage rating greater than 1,4 kV;
b. Energy storage greater than 10 J;
c. Capacitance greater than 0,5 μF; and
d. Series inductance less than 50 nH; or
2. a. Voltage rating greater than 750 V;
b. Capacitance greater than 0,25 μF; and
c. Series inductance less than 10 nH;
b. Superconducting solenoidal electromagnets having all of the following characteristics:
1. Capable of creating magnetic fields greater than 2 T;
2. A ratio of length to inner diameter greater than 2;
3. Inner diameter greater than 300 mm; and
4. Magnetic field uniform to better than 1 % over the central 50 % of the inner volume;
Note: I.3A.003.b. does not prohibit magnets specially designed for and exported ‘as parts of’ medical nuclear magnetic resonance (NMR) imaging systems. The phrase ‘as part of’ does not necessarily mean physical part in the same shipment; separate shipments from different sources are allowed, provided the related export documents clearly specify that the shipments are dispatched ‘as part of’ the imaging systems.
c. Flash X-ray generators or pulsed electron accelerators having either of the following sets of characteristics:
1. a. An accelerator peak electron energy of 500 keV or greater but less than 25 MeV; and
b. With a ‘ figure of merit ’ (K) of 0,25 or greater; or
2. a. An accelerator peak electron energy of 25 MeV or greater; and
b. A ‘ peak power ’ greater than 50 MW.
Note: I.3A.003.c. does not prohibit accelerators that are component parts of devices designed for purposes other than electron beam or X-ray radiation (electron microscopy, for example) nor those designed for medical purposes:
Technical Notes: 1. The ‘ figure of merit ’ K is defined as: K = 1,7 × 10 3 V 2,.65 Q
V is the peak electron energy in million electron volts.
If the accelerator beam pulse duration is less than or equal to 1 μs, then Q is the total accelerated charge in Coulombs. If the accelerator beam pulse duration is greater than 1 μs, then Q is the maximum accelerated charge in 1 μs.
Q equals the integral of i with respect to t, over the lesser of 1 μs or the time duration of the beam pulse (Q = ∫ idt), where i is beam current in amperes and t is time in seconds.
2. ‘ Peak power ’ = (peak potential in volts) × (peak beam current in amperes). 3. In machines based on microwave accelerating cavities, the time duration of the beam pulse is the lesser of 1 μs or the duration of the bunched beam packet resulting from one microwave modulator pulse. 4. In machines based on microwave accelerating cavities, the peak beam current is the average current in the time duration of a bunched beam packet |
I.3A.004 | 3A225 | Frequency changers or generators, other than those specified in I.0A.002.b.13., having all of the following characteristics:
a. Multiphase output capable of providing a power of 40 W or greater;
b. Capable of operating in the frequency range between 600 and 2 000 Hz;
c. Total harmonic distortion better (less) than 10 %; and
d. Frequency control better (less) than 0,1 %.
Technical Notes: Frequency changers in I.3A.004 are also known as converters or inverters.
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I.3A.005 | 3A226 | High-power direct current power supplies, other than those specified in I.0A.002.j.6., having both of the following characteristics:
a. Capable of continuously producing, over a time period of 8 hours, 100 V or greater with current output of 500 A or greater; and
b. Current or voltage stability better than 0,1 % over a time period of 8 hours
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I.3A.006 | 3A227 | High-voltage direct current power supplies, other than those specified in I.0A.002.j.5., having both of the following characteristics:
a. Capable of continuously producing, over a time period of 8 hours, 20 kV or greater with current output of 1 A or greater; and
b. Current or voltage stability better than 0,1 % over a time period of 8 hours.
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I.3A.007 | 3A228 | Switching devices, as follows:
a. Cold-cathode tubes, whether gas filled or not, operating similarly to a spark gap, having all of the following characteristics:
1. Containing three or more electrodes;
2. Anode peak voltage rating of 2,5 kV or more;
3. Anode peak current rating of 100 A or more; and
4. Anode delay time of 10 μs or less;
Note: I.3A.007 includes gas krytron tubes and vacuum sprytron tubes.
b. Triggered spark-gaps having both of the following characteristics:
1. An anode delay time of 15 μs or less; and
2. Rated for a peak current of 500 A or more;
c. Modules or assemblies with a fast switching function having all of the following characteristics:
1. Anode peak voltage rating greater than 2 kV;
2. Anode peak current rating of 500 A or more; and
3. Turn on time of 1 μs or less.
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I.3A.008 | 3A229 | Firing sets and equivalent high-current pulse generators as follows:
N.B.: See also Military Goods Controls.
a. Explosive detonator firing sets designed to drive multiple controlled detonators specified in I.3A.011;
b. Modular electrical pulse generators (pulsers) having all of the following characteristics:
1. Designed for portable, mobile, or ruggedized-use;
2. Enclosed in a dust-tight enclosure;
3. Capable of delivering their energy in less than 15 μs;
4. Having an output greater than 100 A;
5. Having a ‘ rise time ’ of less than 10 μs into loads of less than 40 ohms;
6. No dimension greater than 254 mm;
7. Weight less than 25 kg; and
8. Specified for use over an extended temperature range 223 K (– 50 °C) to 373 K (100 °C) or specified as suitable for aerospace applications.
Note: I.3A.008.b. includes xenon flash lamp drivers.
Technical Notes: In I.3A.008.b.5. ‘ rise time ’ is defined as the time interval from 10 % to 90 % current amplitude when driving a resistive load
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I.3A.009 | 3A230 | High-speed pulse generators having both of the following characteristics:
a. Output voltage greater than 6 V into a resistive load of less than 55 ohms, and
b. ‘ Pulse transition time ’ less than 500 ps.
Technical Note: In I.3A.009, ‘ pulse transition time ’ is defined as the time interval between 10 % and 90 % voltage amplitude
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I.3A.010 | 3A231 | Neutron generator systems, including tubes, having both of the following characteristics:
a. Designed for operation without an external vacuum system; and
b. Utilizing electrostatic acceleration to induce a tritium-deuterium nuclear reaction
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I.3A.011 | 3A232 | Detonators and multipoint initiation systems, as follows:
N.B.: See also Military Goods Controls.
a. Electrically driven explosive detonators, as follows:
2. Exploding bridge wire (EBW);
4. Exploding foil initiators (EFI);
b. Arrangements using single or multiple detonators designed to nearly simultaneously initiate an explosive surface over greater than 5 000 mm 2 from a single firing signal with an initiation timing spread over the surface of less than 2,5 μs.
Note: I.3A.011 does not prohibit detonators using only primary explosives, such as lead azide.
Technical Note: In I.3A.011 the detonators of concern all utilise a small electrical conductor (bridge, bridge wire or foil) that explosively vapourises when a fast, high-current electrical pulse is passed through it. In nonslapper-types, the exploding conductor starts a chemical detonation in a contacting high-explosive material such as PETN (Pentaerythritoltetranitrate). In slapper detonators, the explosive vapourisation of the electrical conductor drives a flyer or slapper across a gap and the impact of the slapper on an explosive starts a chemical detonation. The slapper in some designs is driven by a magnetic force. The term exploding foil detonator may refer to either an EB or a slapper-type detonator. Also, the word initiator is sometimes used in place of the word detonator
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I.3A.012 | 3A233 | Mass spectrometers, other than those specified in I.0A.002.g., capable of measuring ions of 230 atomic mass units or greater and having a resolution of better than 2 parts in 230, as follows, and ion sources therefor:
a. Inductively coupled plasma mass spectrometers (ICP/MS);
b. Glow discharge mass spectrometers (GDMS);
c. Thermal ionization mass spectrometers (TIMS);
d. Electron bombardment mass spectrometers which have a source chamber constructed from, lined with or plated with materials resistant to UF 6 ;
e. Molecular beam mass spectrometers having either of the following characteristics:
1. A source chamber constructed from, lined with or plated with stainless steel or molybdenum and equipped with a cold trap capable of cooling to 193 K (– 80 °C) or less; or
2. A source chamber constructed from, lined with or plated with materials resistant to UF 6 ;
f. Mass spectrometers equipped with a microfluorination ion source designed for actinides or actinide fluorides.
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