Thanks Frank,
Glad I haven't missed any too obvious discussions then.
Yes, agreed, Drift and TC need to be considered separately but I don't think moving from active heating to passive TC compensation should adversely affect drift. With well aged external resistors and low overall power dissipation (eg, no op-amp and transistor drive for the heater) hopefully at room temperature drift would be very low indeed.
For the TC, I'm not sure if your 50ppm/°C includes the Vbe of the compensating transistor or not, I'm assuming that it does (I can't find a figure in the datasheet). That particular application circuit seems to be tweaking the zener current to optimise the tracking of the zener and compensation transistor TCs (hopefully by shunting a 200R long term stable resistor with a high value less critical shunt one). It's a question of how close that tracking / compensation can get over a limited (room) temperature range, which it sounds as if nobody's really looked into.
It also occurs to me that if the heater is not in active use then there is also the sense transistor available which could maybe be employed in a second order compensation circuit?
At least having the on-chip heater would make the thermal cycling nice and easy for trimming... and maybe for 'relaxing' any hysteresis too.
Of course I don't actually have an LTZ1000 but the possibility is making me edge towards about a Digikey order!
EDIT: Though I suppose if adverse effect on drift is already so low when heated, then there may not be too much milage in this approach. I just like the elegance of a room temperature solution that doesn't have as many issues with thermocouple effects with a heated package.
Well, afair, it is nearly impossible for the LTZ reference, to trim its T.C. (unheated, of course superposition of zener and BE diode) to near zero.
Therefore, a room temperature solution w/o oven is absolutely wishful thinking.
The other Fluke topology, i.e. BE diode on top of the zener, that is SZA263 and LTFLU, they may be really trimmed to near zero T.C.
Fluke used that feature in the 731B, transfer standard, and in the 5200A, AC standard.
But these achieve 1 ppm/°C at best, and maybe the initial T.C. trimming may not last forever.
So you may try that, but such a solution has nothing to do with an Ultra Precision voltage standard, as we discussed here.
W/o an oven, you simply cannot achieve ultra high stability with Reference Amplifiers.
It is also worthless to make things complicated.
With the intended mechanism (oven), stable resistors, and a LTZ1000CH at 45°C, with the simplest circuit possible, you will definitely achieve stabilities in time and temperature, which you will have big difficulties to verify with amateur based tools.
Thermo voltages are also not a problem at all with proper layout and thermo-mechanical setup.
The existence of all these ovenized references and standards are a simple proof for that!
The LTZ oven is not a good choice for temperature cycling, if you have a relatively low oven temperature.
This cycling, intended to remove hysteresis, only works correctly, if you have a symmetrical temperature swing below and above the stabilization temperature.
With 45°C, you may cycle between 25°C (r.t.) and 65°C. For these low temperatures, you might see no hysteresis at all, it's simply not working.
So you might select 65°C, to have a +/- 40°C swing, but this setting increases the timely drift, as a big disadvantage.
At 45°C, you may try to avoid any excess temperature of the LTZ, or do the temperature cycling of the whole assembly from 0°C to +90°C, in a climate chamber.
Frank