Sal

joined 3 years ago
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[–] Sal@mander.xyz 1 points 2 months ago (9 children)

Thanks a lot! I can understand some of what I am looking at now.

I would like to find out if there are associated phenomena that I might be able to notice using software-defined radio. Maybe some time I can chase after an aurora, but this time I am unprepared.

[–] Sal@mander.xyz 1 points 2 months ago (4 children)

Very interesting indeed! Unfortunately I was not able to catch up with the jargon before the flux rope with a stable positive Bz component arrived, so I am not yet quite sure what that means, but I hope it turns southwards 😛

Going through charts, I see that a lot have very short time cut-offs. At most I see data from 2 days back, so I don't know if the numbers I see in the charts are special or not... Do you know if there is a way to see historical data plots of these values?

[–] Sal@mander.xyz 1 points 2 months ago (6 children)

Wow! Major solar fireworks today. Charge your camera batteries and put on your finest jacket for tomorrow night as strong (G3) or perhaps even severe (G4) geomagnetic storm conditions are possible tomorrow evening (1 June) into 2 June.

I learn about an astronomical event BEFORE it happens?! Pretty exciting, I often learn about space events after they already happened 😆 Now I even get a few hours to prepare.

Is there some sensor that I can use to detect this? Will it produce some characteristic radio signal or X-ray pattern? How do I tune in?

[–] Sal@mander.xyz 1 points 2 months ago
[–] Sal@mander.xyz 8 points 2 months ago

Wow, a really nice shot of a really nice frog!

[–] Sal@mander.xyz 4 points 2 months ago

Happy you find it useful! I added the images that went into the stack for reference just now.

[–] Sal@mander.xyz 2 points 2 months ago

Oh, wow! I didn't know about this microscopic difference between monocots and dicots. So cool!

[–] Sal@mander.xyz 2 points 2 months ago

You are a radical vegan

[–] Sal@mander.xyz 2 points 2 months ago

that was a bit confusing at first (where is the crop factor!), i have never really messed with by-x lenses

Haha, I think I have a good idea of why.... When thinking about general photography, common scenes involve many different types of objects of varying sizes and distances. In this context it makes sense to define the "field of view" of a lens in terms of the visual angle, and to think about differences between equipment in terms of a "reference" - that's where the 'crop factor' comes in, when comparing to a 35 mm film as a standard to measure relative to. It is a bit silly to ask a question such as "how many cats can fit into the image that gets projected into the camera sensor?"

When one gets into macro photography things start changing. The distances between the camera and the subjects are defined more narrowly and the size of the subjects one tries to capture is closer in size to the camera sensor's size. In macro-photography you hear about things like a "1:1" lens, meaning that the image of an object placed at a specific distance will be replicated 1:1 at the camera sensor's position. It becomes then meaningful to think about the camera sensor size in absolute sense, because a sensor will capture a scene of its own size (for 1:1). You can still think in relative terms using the crop factor, but it is not as useful to make relative comparisons anymore because the absolute scale is already giving us information that we can work with directly.

For microscopy this trend continues - the distance to the subject is well-defined and we can think in absolute terms about the magnification of the image that gets projected into camera sensor.

Then i got sidetracked on how microscope rulers are being made.

I have not looked into this! I am not sure.... I will look it up.

I reckon you have your setup calibrated.

I do have a ruler but I misplaced it and I have not used it in a while. So, not really, I wouldn't say it is "calibrated". I did take some photos of the ruler that I can use to get a good rough estimate if I can find them.

[–] Sal@mander.xyz 8 points 2 months ago (1 children)

Unfortunately the universe consists of mostly empty space and the infinitely thin cut passess between sub-atomic particles, barely tickling the vacuum fluctuations

[–] Sal@mander.xyz 5 points 2 months ago

Vaccines cure autism

[–] Sal@mander.xyz 2 points 2 months ago

But a sociopath

 

Abstract

Efficient single-photon generation remains a big challenge in quantum photonics. A promising approach to overcome this challenge is to employ active multiplexing—repeating a nondeterministic photon pair generation process across orthogonal degrees of freedom and exploiting heralding to actively route the heralded photon to the desired single output mode via feedforward. The main barriers of multiplexing schemes, however, are minimizing resource requirements to allow scalability and the lack of availability of high-speed, low-loss switches. Here, we present an on-chip temporal multiplexing scheme utilizing thin-film lithium niobate (TFLN) photonics to effectively address these challenges. Our time-multiplexed source, operating at a rate of 62.2 MHz, enhances single-photon probability by a factor of 3.37 ± 0.05 without introducing additional multi-photon noise. This demonstration highlights the feasibility and potential of TFLN photonics for large-scale complex quantum information technologies.

11
submitted 6 months ago* (last edited 6 months ago) by Sal@mander.xyz to c/biology@mander.xyz
 

Abstract: Miniaturization of mid-infrared (MIR) spectroscopy sources has progressed signifi- cantly during the past two decades, but a solution able to provide full integration, high optical power and wide tuneability in the so-called atmospheric window (2.5 - 5 μm) is still missing. In this context, we investigated a broadband frequency-tuneable source relying on difference frequency generation (DFG) in a periodically poled lithium niobate (PPLN) ridge waveguide. By employing tuneable lasers for the pump and signal wavelengths emitting at around 1 μm and 1.55 μm, respectively, we were able to fully cover the ≈ 3 - 3.5 μm spectrum, thus translating the technological maturity of data communication photonic sources to the MIR wavelength band.

Moreover, the use of a relatively large cross-section for the here proposed PPLN ridge waveguide compared to commonly employed thin-film lithium niobate (TFLN) waveguides has allowed us to achieve low propagation and coupling losses together with high damage threshold, thereby allowing us to reach mW-level power in the MIR wavelength band.

9
submitted 6 months ago* (last edited 6 months ago) by Sal@mander.xyz to c/mander@mander.xyz
 

Edit: The issue appears to have been some intermittent problem and it was solved (perhaps by chance) a few minutes after contacting support.

I woke up this morning to find out that the images are not accessible through the site.

This seems to be an issue on the side of the object storage provider, as the "bucket" is not accessible through the provider's web portal. I have reached out to them to hopefully sort this out ASAP.

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