2 mm 12-well Comb RS 2392064.

AE-6210 Slab Gel Cast

Reason and Application
Gel projecting unit for Slab size (138 x 130 mm, thickness 1 mm or 2 mm) gel

Highlights

Simple setting with uniquely planned parts and seal gasket
Simple gathering by putting a couple of glass plates and a seal gasket together in the set position
Indeed, even a novice can hand cast a gel without hole or channel
Prepared to project a gel of 1 to 2.0 mm thickness
Viable electrophoresis device: ATTO Slab Gel Electrophoresis System (AE-6220 Dual Slab Chamber).

0.75 mm Compact Multi Gel Cast
Portrayal: I ncl udi ng 2 pai r s of gl ass pl at es, 2 brushes, 3di vi der pl at e and 1 faker pl at e. Prepared t o cast t wo 12-wel l gel s

Void Gel Cassette Combs, small scale, 1.0 mm, 12 well

These looks over are for use while pouring your own extraordinary gel types and are accessible in two thicknesses (1.0 mm and 1.5 mm) and seven well arrangements (1 well, 2 well, 5 well, 10 well, 12 well, 15 well, and 2D well). They are viable with our little size Empty Gel Cassettes of a similar thickness (NC2010, 1.0 mm; NC2015, 1.5 mm).

Theoretical and Figures

The activity of a recurrence brush at outrageous bright (XUV) frequencies in light of pair-wise intensification and nonlinear upconversion to the fifteenth symphonious of heartbeats from a recurrence brush laser in the close infrared reach is accounted for.

Following a first record of the investigation [Kandula et al., Phys. Fire up. Lett. 105, 063001 (2010)], a broad audit is given of the exhibition that the subsequent range at 51 nm is completely stage intelligent and can be applied to accuracy metrology. The beats are utilized in a plan of direct-recurrence brush excitation of helium iotas starting from the earliest stage to the 1s4p and 1s5p 1P_1 states.

Laser ionization by helper 1064 nm beats is utilized to identify the energized state populace, bringing about a cosine-like sign as a component of the redundancy pace of the recurrence brush with a regulation difference of up to 55%. Investigation of the perceivability of this brush structure yields an expected timing jitter between the two upconverted brush laser beats of 50 attoseconds, whch demonstrates that augmentation to significantly more limited frequencies ought to be possible.

The helium metrology examination brings about change frequencies of 5740806993(10) MHz and 5814248672(6) MHz for excitation of the 1s4p and 1s5p 1P_1 states, separately. This establishes the principal outright recurrence estimation in the XUV, achieving extraordinary exactness in this austere piece of the electromagnetic range.

From the deliberate change frequencies an eight-overlap further developed 4He ionization energy of 5945204212(6) MHz is inferred. Additionally another incentive for the 4He ground state Lamb shift is found of 41247(6) MHz. This trial esteem is in concurrence with ongoing hypothetical computations up to arrange m\alpha^6 and m^2/(M\alpha^5), however with a six times higher accuracy, therewith giving a tough trial of quantum electrodynamics in bound two-electron frameworks.

XUV recurrence brush metrology on the ground condition of helium.

The activity of a recurrence brush at outrageous bright (XUV) frequencies in view of pair-wiseamplification and nonlinear upconversion to the fifteenth consonant of heartbeats from a recurrence comblaser in the close infrared reach is accounted for.

Following a first record of the examination [Kandula etal., Phys. Fire up. Lett. 105, 063001 (2010)], a broad survey is given of the exhibit that theresulting range at 51 nm is completely stage lucid and can be applied to accuracy metrology.

The pulses are utilized in a plan of direct-recurrence brush excitation of helium particles from the groundstate to the 1s4pand 1s5p1P1states. Laser ionization by assistant 1064 nm beats is utilized to detectthe energized state populace, bringing about a cosine-like sign as a component of the redundancy rate ofthe recurrence brush with a regulation difference of up to 55%.

Examination of the perceivability of this combstructure, subsequently involving the helium molecule as an accuracy stage ruler, yields an expected timing jitterbetween the two upconverted brush laser beats of 50 attoseconds, which is identical to a stage jitterof 0.38(6) cycles in the XUV at 51 nm. This sets a quantitative figure of legitimacy for the operationof the XUV brush, and shows that expansion to much more limited frequencies ought to be feasible.The helium metrology examination brings about change frequencies of 5740806993(10) MHz and5814248672(6) MHz for excitation of the 1s4pand 1s5p1P1states, individually.

1 mm 12-well Comb, RS
2392061	Atto	3unit	333.6 EUR
2 mm 12-well Comb, RS
2392064	Atto	3unit	333.6 EUR
1 mm 6-well Comb, RM
2328375	Atto	3unit	306 EUR
1 mm 8-well Comb, RM
2328376	Atto	3unit	306 EUR
1 mm 8-well Comb, RS
2392060	Atto	3unit	333.6 EUR
1 mm 20-well Comb, RM
2328422	Atto	3unit	373.2 EUR
1 mm 10-well Comb, RM
2328948	Atto	3unit	345.6 EUR
1 mm 20-well Comb, RS
2392062	Atto	3unit	333.6 EUR
2 mm 8-well Comb, RS
2392063	Atto	3unit	333.6 EUR
2 mm 20-well Comb, RS
2392065	Atto	3unit	333.6 EUR
1 mm 12-well Combs 2/pk, RM(RMS 10-12)
2398269	Atto	5unit	326.4 EUR
0.75 mm 12-well Combs 2/pk, CP
2393640	Atto	5unit	308.4 EUR
6-well comb, 1mm
2398206	Atto	3unit	303.6 EUR
1.5mm 6-well Comb
2398297	Atto	8unit	300 EUR
9-well comb, 1mm
2398319	Atto	3unit	346.8 EUR
10-well comb, 1mm
2398207	Atto	3unit	303.6 EUR
14-well comb, 1mm
2398213	Atto	3unit	303.6 EUR
15-well comb, 1mm
2398317	Atto	3unit	376.8 EUR

This constitutesthe first outright recurrence estimation in the XUV, accomplishing uncommon precision in thiswindowless piece of the electromagnetic range. From the deliberate change frequencies aneight-overlay further developed 4He ionization energy of 5945204212(6) MHz is inferred. Likewise another worth forthe 4He ground state Lamb shift is found of 41247(6) MHz. This exploratory worth is in agreementwith ongoing hypothetical computations up to arrange mα6and m2/Mα5, however with a six times higherprecision, therewith giving a severe trial of quantum electrodynamics in bound two-electronsystems.