AKADEMİSYENLER VE DOKTORA ÖĞRENCİLERİNİN HEP KULLANDIĞI AMA HERKES BİLSİN İSTEMEDİĞİ SİTELER.
Bunu kaydedin mutlaka. Akademik anlamda sürekli ödeme yapmanıza gerek yok. Aşağıdaki siteler size fazlasıyla yetecek.
1. https://t.co/AiiUAUM75I
Dünyanın en büyük açık kütüphanesi. Profesörünüzün atadığı neredeyse her ders kitabı burada ücretsiz olarak mevcut.
2. https://t.co/lxrqkX8FtH
Akademik makaleler için arama motoru. En etkili araştırmaları bulmak için atıflara göre sıralayın.
3. https://t.co/rexxn41f8R
Akademik tez ve makale üretim motoru. Sıfır halüsinasyonla bölüm yazımı.
4. https://t.co/9AcMjHxGwm
Allen Enstitüsü tarafından geliştirilen yapay zeka destekli makale arama. Her atıfı bağlamında vurgular.
5. https://t.co/1pUSgSdS6D
Bir makaleyi girin, her ilgili çalışmayı bir grafik olarak haritalanmış görün. Uzmanların gerçekten birlikte okuduğu şeyleri ortaya çıkarır.
6. https://t.co/tHPqEh4Jfa
Bir yapay zeka araştırma asistanı. Herhangi bir soruyu sorun ve ana bulgularla birlikte yapılandırılmış makale tabloları alın.
7. https://t.co/iQBF4OKvAL
Binlerce makalenin sonuçlarını tek bir cevapta birleştirir. Kiraz seçmeyi önler.
8. https://t.co/FGPnpvrhZy
Makalelerin Spotify'si. Zaten okuduklarınıza dayanarak yeni araştırmalar önerir.
9. https://t.co/Hvs7besTv6
Atıf zincirlerini görselleştirir. Bir fikrin on yıllar süren araştırmalarda nasıl yayıldığını gösterir.
10. https://t.co/Pl3X0YIvIg
Hangi makalelerin herhangi bir iddiayı desteklediğini, çürüttüğünü veya bahsettiğini söyler. Saatlerce gerçeklik kontrolü yapmaktan tasarruf sağlar.
11. https://t.co/r7BhsKSHp7
200 milyon açık erişimli makale tek bir aranabilir indekste. Dünyanın en büyük ücretsiz akademik arşivi.
"Matrix Calculus for Machine Learning and Beyond" is an interesting set of free lecture notes for understanding the mathematics behind modern deep learning. It covers gradients, Jacobians, Hessians, matrix-valued functions, backpropagation, optimisation, and many of the mathematical structures used in machine learning and AI models.
One interesting aspect is that the material maintains a strong university-level rigour while remaining highly visual: the notes include numerous diagrams, graphs, geometric interpretations, and intuitive explanations of matrix calculus applied to neural networks.
It is a valuable resource not only for students studying machine learning, but also for anyone who wants to build a solid foundation in computational linear algebra and optimisation.
https://t.co/XsnReRHu35
Teichmüller Space is a central object in geometry and complex analysis. It describes all possible geometric structures of a surface, up to smooth deformation. Originally developed in topology and Riemann surface theory, it studies how shapes can change while preserving intrinsic conformal properties.
In machine learning, Teichmüller geometry has become relevant in geometric learning and manifold-based representation. Many datasets lie on nonlinear manifolds rather than Euclidean space, and Teichmüller tools help understand shape-preserving embeddings, geometric feature extraction, and structured latent spaces.
In deep learning, it appears in geometric deep learning, graph embeddings, and shape analysis. Surface matching, medical imaging, 3D vision, and mesh learning often rely on conformal mappings closely related to Teichmüller theory.
In reinforcement learning, Teichmüller-inspired geometry can help in navigation on curved spaces, continuous control, and manifold optimization. The deeper idea is that learning often happens not in flat vector spaces, but on curved geometric structures, where understanding the geometry of deformation becomes crucial.
In flow matching, a coupling determines how noise and data samples are paired during training.
The choice of coupling is important because it influences the geometry of trajectories at inference time.
The simplest choice is the independent coupling, where noise and data points are paired arbitrarily. This can lead to curved trajectories as the model averages over many conflicting pairings.
However, if we use optimal transport on batches of pairs, this leads to fewer ambiguous intersections that the model must resolve, leading to straighter trajectories at inference time.
The Helmholtz decomposition is one of the fundamental results of vector calculus.
It says any well-behaved vector field can be split into two parts, one capturing sources and sinks through divergence, and one capturing rotation through curl.
Final Lecture of our Statistical Mechanics Series.
Lecture 2 showed how we move from the Full Phase-Space Density
ρ(q₁, …, qₙ, p₁, …, pₙ, t)
to smaller statistical objects by integrating out variables we do not want to keep. That gives reduced descriptions like the One-Particle Density
f₁(q₁,p₁,t)
and the Two-Particle Density
f₂(q₁,p₁,q₂,p₂,t)
This was the simplification.
Now comes the catch.
If the Full Density obeys Liouville’s Equation, the reduced densities do not evolve independently. The equation for one level depends on the next one and this is referred to as the BBGKY hierarchy.
The One-Particle Density depends on the Two-Particle Density.
The Two-Particle Density depends on the Three-Particle Density.
And the chain keeps going.
That happens because particles interact. Once one particle feels the rest, one-particle information is no longer enough. Correlations enter, and the lower level is fed from above.
If the full Hamiltonian is
H = Σᵢ pᵢ²/(2m) + Σᵢ U(qᵢ) + (1/2) Σᵢ Σⱼ≠ᵢ Φ(qᵢ − qⱼ)
then reducing the full density does not make the interaction terms disappear. It leaves behind coupling to higher-order reduced densities. So, schematically,
∂f₁/∂t + transport of one particle = interaction term involving f₂
and more generally the heirarchy is such that
∂fₛ/∂t + s-particle transport = interaction term involving fₛ₊₁
Therefore, Lecture 3 is really about the price of reduction. We simplify the description, but the information we remove comes back as coupling to higher-order correlations.
So, how do you actually compute anything if every level depends on the next one?
This is the so-called Closure Problem.
To make the hierarchy usable, you need an extra assumption that cuts the chain. You replace the exact higher-order object by an approximation in terms of lower-order ones. The most basic example is a factorized closure at the pair level, where the exact correlated Two-Particle Density is replaced schematically by a product of One-Particle Densities:
f₂(q₁,p₁,q₂,p₂,t) ≈ f₁(q₁,p₁,t) f₁(q₂,p₂,t)
That approximation is not exact. It throws away part of the correlation structure. But it gives you something the raw hierarchy does not... a closed equation for the lower-level description.
That is why closure matters so much. Without it, the hierarchy is exact but open. With it, the theory becomes approximate but usable.
Thus, the combined point of this final Statistical Mechanics post is simple.
First, reduced descriptions are not closed because interactions generate correlations across levels.
Second, if you want a workable Kinetic Theory, you must close the hierarchy by approximating those higher-order correlations.
It is the bridge from formal many-body mechanics to equations people can actually solve.
In the render, that is exactly the story you are seeing. The first part shows the hierarchy itself: one reduced level feeding the next, with lower descriptions inheriting structure from higher ones. The second part shows the closure step where the exact correlated pair level is replaced by a factorized ansatz, and that approximation gives back a closed one-particle description. That is, the animation moves from dependence to approximation, and from approximation to solvability.
#StatisticalMechanics #BBGKY #ClosureProblem #KineticTheory #PhaseSpace #ReducedDistribution #HamiltonianMechanics #MathematicalPhysics #Mathematics #Physics
In physics tesseract is used to model higher dimensional spaces, such as in theoretical physics, cosmology (e.g., studying dark energy), and general relativity.
One equation generates all of reality. The Lagrangian ℒ = T − V — kinetic minus potential energy — is the seed. Feed it a symmetry group and it tells you which universe you get. U(1) gives you light. SU(3) gives you confinement. SU(2)×U(1) gives you mass via the Higgs. The entire Standard Model — every force, every particle, every interaction — is just one Lagrangian density with the gauge group SU(3) × SU(2) × U(1). I made this infographic to show what most physics education never makes visual: the deep structure is a single equation that branches into all of physical reality based on which symmetry you choose. Nature doesn’t pick forces. It picks symmetries. The forces are consequences.
Divergence and curl are complementary concepts from vector calculus.
Divergence quantifies the rate at which a field flows outward from a point and curl represents rotation.
A single vector field can have both divergence and curl, leading to an outward spiral pattern.