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Show & Tell PUBLIC

Built something cool in the Quantum Quest simulator? Post it here โ€” polished experiments, happy accidents, and total mysteries all welcome. The ๐Ÿ“ธ Community button in the simulator drops your circuit straight into this group.

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๐Ÿ“Œ HOW THIS GROUP WORKS

This is the place to show off what you build in the Quantum Quest simulator โ€” polished experiments, happy accidents, and total mysteries all welcome.

The easy way to post here: build something in the simulator, hit the ๐Ÿ“ธ Community button, and your circuit snapshot lands here automatically.

When you share, tell us two things:
1. What you were trying to do
2. What actually happened

Questions and "how did you do that?" comments are the whole point. Be generous with likes โ€” someone's first circuit is a big deal.

โ€” The Quantonic Team
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DONE WITH THE TOUR? ๐Ÿ—บ๏ธ

If you've tried the circuits in this group, you're past the beginner wall. Next stops: the guided lessons (13 of them, step-checked), the Challenges tab for instant feedback, and the Weekly Challenges group for fresh puzzles.

And whatever you build โ€” ๐Ÿ“ธ it back here. Someone's always stuck exactly where you just were.

โ€”โ€”โ€”
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Q0 OR Q1? THE ETERNAL QUESTION ๐Ÿ”ข

Run X on qubit 0 alone, screenshot it. Run X on qubit 1 alone, screenshot that.

Which digit moved each time? Leftmost = qubit 0, here and in the results. Do this drill once and the convention never bites you again.
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THE IDENTITY GAME ๐Ÿƒ

Challenge: build the LONGEST circuit that provably does nothing. XX, HH, SWAPยทSWAP, HZHยทXโ€ฆ

Post your do-nothing masterpiece with its histogram as proof. Silliest circuit that still returns 100% |0โŸฉ wins the comments.

โ€”โ€”โ€”
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TWO SWAPS = NOTHING ๐Ÿ”„

X on qubit 0, then SWAP, then SWAP again. Back exactly where you started.

Sounds obvious โ€” but it's your reversibility instinct in training. Every gate has an undo; find the undo for S. (It isn't S.)
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RUN YOUR OWN BELL TEST ๐Ÿงช

Make the Bell pair and run 1000 shots. Count how often the two digits agree: 100%.

Now X-basis them (H on both before measuring): still perfectly correlated. Agreement that survives a basis change is the real spooky part.

โ€”โ€”โ€”
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SHARE YOUR FAIL ๐Ÿ’ฅ

Standing invitation: post the circuit that did NOT do what you wanted.

Wrong histogram, mystery bar, gate that seemed to do nothing โ€” the debugging conversation is usually more educational than the victory lap.
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WHY REAL HARDWARE RACES THE CLOCK โณ

In this simulator your qubits wait patiently forever. Real ones don't โ€” the environment "measures" them uninvited within microseconds. That's decoherence.

Every circuit you build here would be a sprint against that clock on real metal. Enjoy the luxury.

โ€”โ€”โ€”
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THE 3-2-1 CHALLENGE ๐Ÿ

Three qubits. TWO gates. Histogram must show exactly two outcomes.

There's more than one answer โ€” post yours and compare. (If you found three gates first, that's the famous one; the two-gate version is sneakier.)
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S VS Z: THE SHOWDOWN ๐ŸฅŠ

Start with H. Then EITHER S or Z. Then H again.

The Z version lands on 1 with certainty; the S version stays 50/50. Two "invisible" phase gates, completely different fingerprints once interference gets involved.

โ€”โ€”โ€”
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GUESS THE HISTOGRAM #4 ๐Ÿค”

H on qubit 0, then SWAP qubits 0 and 1.

Where does the randomness live now? Predict which digit wobbles before you run it. SWAP moves states, not labels.
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A GENUINE RANDOM NUMBER ๐ŸŽฐ

Three H gates, three measurements: a true 3-bit random number, 0โ€“7, from physics rather than arithmetic.

Commercial quantum random number generators are essentially this circuit with better packaging. Yours is free.

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THE STAIRCASE ๐Ÿชœ

X on qubit 0, CNOT 0โ†’1, CNOT 1โ†’2. The 1 cascades down the wires: 111, every time.

Now replace the X with H and run it again โ€” deterministic staircase becomes entangled triplet. One gate swap, whole new physics.
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FLIP HALF THE PACT ๐Ÿช™๐Ÿ”—

Make a Bell pair, then put a Z on just one of the qubits.

The histogram doesn't budge โ€” still 00 and 11. The phase changed sides invisibly. (In the X basis it's a different story โ€” H both qubits before measuring and compare.)

โ€”โ€”โ€”
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Admin QuantonicHQ
MAKE '01' FROM SCRATCH ๐Ÿงฉ

Tiny drill: produce exactly the outcome 01, with certainty.

Sounds trivial โ€” but which qubit gets the X? (Leftmost digit is qubit 0.) Thirty seconds of practice that saves you an hour of confusion later.
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WHY SHOTS AT ALL? ๐ŸŽฏ

The simulator could just print the exact probabilities โ€” real quantum hardware can't. One run yields one sample, full stop.

That's why every real algorithm is designed around statistics, and why the shots slider is the most honest control in the app.

โ€”โ€”โ€”
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ONE WIRE, BIG LESSONS 1๏ธโƒฃ

Set the simulator to a single qubit and go gate by gate: X, H, Z, S, T, the rotations.

Most "what does this gate DO" confusion dissolves when there's only one wire to watch. Post the histogram that surprised you most.
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THE GATE YOU CAN'T SEE (PART 2) ๐ŸŒ€

RZ rotates around the Z axis โ€” and in the standard histogram, NOTHING changes, at any angle.

Sandwich it in H gates and the rotation becomes visible. A histogram is one shadow of the state, never the whole shape.

โ€”โ€”โ€”
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BUILD A PARITY CHECKER โœ…

CNOT qubit 0 โ†’ qubit 2, then CNOT qubit 1 โ†’ qubit 2. Qubit 2 now answers one question: is the number of 1s odd?

Test it on all four inputs. Parity checks like this are the atoms of quantum error correction.
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INTERFERENCE IS SUBTRACTION โž–

H then H again: back to certain 0. But WHY?

After the first H there are two paths to "1" โ€” and their amplitudes are equal and OPPOSITE. They cancel. Quantum computing is the art of arranging these cancellations on purpose.

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GUESS THE HISTOGRAM #3 ๐Ÿค”

X on qubit 0, then SWAP the two qubits.

Which label lights up โ€” 10 or 01? This one is pure ordering-convention practice (leftmost digit = qubit 0). Predict, run, post.
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XOR IN ONE GATE โŠ•

Set the two inputs with X gates (or don't), then CNOT into the target: the target now holds input-1 XOR input-2.

Try all four input combos and check the truth table. Quantum computers contain ordinary logic โ€” it's the superposition on top that's new.

โ€”โ€”โ€”
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PRESET TOUR: COINFLIP ๐Ÿช™

The humble coinflip preset โ€” one H, one measurement. It's the soundcheck of quantum computing.

If you've never shared a circuit before, run this one, hit ๐Ÿ“ธ, and make it your first post. Everyone starts here.
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THE COPY THAT ISN'T ๐Ÿšซ๐Ÿ“‹

CNOT copies classical bits perfectly: 0โ†’00, 1โ†’11. So put the control in superposition (H first) and you get... two copies of the superposition?

No โ€” you get entanglement instead. Quantum states can't be cloned, and this two-gate circuit is the proof.

โ€”โ€”โ€”
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EIGHT BARS ๐Ÿ“Š

Three qubits, one H on each: eight outcomes, equal heights.

Every H doubles the possibilities โ€” ten qubits would give 1024 bars. That doubling is exactly why classical computers struggle to keep up. See it with your own eyes at N=3.
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THE SLOW-MOTION FLIP ๐ŸŽฌ

Run RY at a small angle, then bigger, then bigger still, up to a half-turn.

Watch the histogram slide from all-0 through 50/50 to all-1. X isn't an on/off switch โ€” it's the endpoint of a dial you can stop anywhere.

โ€”โ€”โ€”
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GUESS THE HISTOGRAM #2 ๐Ÿค”

H on qubit 0, CNOT 0โ†’1, then X on qubit 1.

Bell pair with a twist โ€” literally. Predict the two surviving outcomes before running. First correct guess in the comments gets bragging rights.
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YOU CAN'T PEEK TWICE ๐Ÿซฃ

Run a circuit, get 0. Run it "again", get 1. Which is right? Both.

Each run creates a fresh superposition and measurement settles it fresh. There is no "the" answer stored inside โ€” that's not noise, that's the physics.

โ€”โ€”โ€”
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BUILD THE ANTI-BELL ๐Ÿ””

Make the classic Bell pair (H, CNOT), then add one X on either qubit.

Now the histogram shows only 01 and 10 โ€” perfect DISagreement. Same entanglement, opposite pact. One gate flipped the contract.
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T: THE EIGHTH TURN โฑ๏ธ

The T gate is the smallest step in the standard family: Tยฒ=S, Tโด=Z, Tโธ = back to the start.

Why care about such a tiny turn? Because with H and T alone you can approximate ANY single-qubit operation. Two gates, the whole sphere.

โ€”โ€”โ€”
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THE S GATE COUNTDOWN ๐Ÿ•

S twice = Z. Z twice = identity. So four S gates in a row do... nothing at all.

Verify with histograms (hint: you'll need the H-sandwich trick to see anything). Gates are clockwork โ€” fractions of a full turn.
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WHERE DID 01 AND 10 GO? ๐Ÿซฅ

In a Bell pair, four outcomes were possible before the CNOT โ€” then two of them vanished.

They didn't get filtered out; their amplitudes simply never formed. Entanglement is bookkeeping with amplitudes, and the missing bars are the receipt.

โ€”โ€”โ€”
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GUESS THE HISTOGRAM #1 ๐Ÿค”

X on qubit 0. H on qubit 1. Nothing else.

Before you run it: how many bars, which labels, what heights? Post your guess in the comments, then your actual histogram. No shame โ€” the ordering convention bites everyone once.
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PHASE KICKBACK, LIVE ๐Ÿชƒ

Put the control in |+โŸฉ (H), the target in |โˆ’โŸฉ (X then H), then CNOT, then H on the control.

The CONTROL comes out as 1 โ€” the target kicked its phase back upstream. This trick powers half the famous algorithms.

โ€”โ€”โ€”
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PRESET TOUR: PLUSMINUS โž•โž–

The plusminus preset prepares |+โŸฉ and |โˆ’โŸฉ โ€” two states with IDENTICAL 50/50 histograms.

Add one H before measuring and suddenly they're perfectly distinguishable: one goes to 0, the other to 1. Basis matters.
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WHY YOUR 50/50 IS 53/47 ๐Ÿ“‰

Ran H and got 53/47? Nothing is broken. Each shot is one coin flip, and 100 flips rarely land exactly even.

Rule of thumb: the wobble shrinks like 1/โˆšshots. Compare 100 shots against 10,000 and watch the bars settle.

โ€”โ€”โ€”
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THE CHAIN REACTION โ›“๏ธ

H on qubit 0, CNOT 0โ†’1, then CNOT 1โ†’2. The middle qubit passes the correlation along like a rumour.

Only 000 and 111 survive. Now move the H to the middle qubit and see what changes โ€” post both.
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ENTANGLED OR JUST RANDOM? ๐Ÿ•ต๏ธ

Circuit A: H on both qubits โ€” four bars.
Circuit B: H then CNOT โ€” two bars.

Both are "random", but B's qubits move as one. The histogram shape is how you tell correlation from coincidence.

โ€”โ€”โ€”
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THE FOUR-SIDED QUANTUM DIE ๐ŸŽฏ

H on each of two qubits: 00, 01, 10, 11 at 25% each.

Simple โ€” but predict it BEFORE you run it. Then ask: are these two qubits entangled? (Hint: no. Tomorrow's histograms will show you why that matters.)
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THE TRIPLET PACT ๐Ÿ”—

H on qubit 0, then CNOT 0โ†’1 and CNOT 0โ†’2. Three qubits, and the histogram shows only 000 and 111.

One random decision, three qubits bound to it. This is the GHZ state โ€” entanglement doesn't stop at pairs.

โ€”โ€”โ€”
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SWAP, BUILT BY HAND ๐Ÿ”€

Three CNOTs, alternating direction: 0โ†’1, 1โ†’0, 0โ†’1. Congratulations, you built SWAP from scratch.

Load the swapdance preset and check your version against it. Same histogram = same circuit.
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LOAD THE DICE ๐ŸŽฒ

An RY gate with a small angle: mostly 0s. Crank the angle: the odds slide continuously toward all 1s.

Probability is amplitude squared โ€” the angle is the knob. Can you hit 70/30?

โ€”โ€”โ€”
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THE H-Z-H SANDWICH ๐Ÿฅช

Run H, Z, H on one qubit starting from 0. You get 1, every single time.

Three gates that equal one X gate โ€” your first taste of the fact that gate sequences multiply like rotations. Prove it side by side and share both histograms.
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THE INVISIBLE GATE ๐Ÿ‘ป

Circuit A: H. Circuit B: H then Z. Identical 50/50 histograms.

So does Z do nothing? Not quite โ€” it flipped the phase, which the histogram can't see. Follow-up post coming on how to catch it red-handed.

โ€”โ€”โ€”
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FLIP IT AND REVERSE IT ๐Ÿ”

Put two X gates in a row. The histogram: 100% back where you started.

Every quantum gate is reversible โ€” nothing is ever "overwritten". Try the same trick with two SWAPs on two qubits.
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TWO COINS, ONE FATE ๐ŸŽญ

H on qubit 0, CNOT to qubit 1. Two "coins", but they always land the same way โ€” 00 or 11, never split.

Neither qubit decided in advance. That's entanglement, and you just made it in two gates.

โ€”โ€”โ€”
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THE ONE-GATE WONDER โœจ

One qubit, one H gate, 1000 shots. That wobbly 50/50 histogram is the whole field in miniature: a deterministic machine producing genuine randomness.

Run it, ๐Ÿ“ธ it, post it โ€” everyone's first circuit belongs here.
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SHOW US YOUR WEIRDEST HISTOGRAM ๐Ÿ“Š

Standing thread: post the strangest measurement histogram you've ever produced โ€” on purpose or by accident.

Bonus points if:
โ€ข You don't know why it looks like that (we'll figure it out together)
โ€ข It looked nothing like what you predicted
โ€ข It's beautiful

There is no wrong answer here. Some of the best physics starts with "huh, that's odd."
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PRESET SPOTLIGHT: SWAP DANCE ๐Ÿ•บ

Open the presets menu in the simulator and load "swapdance".

Watch what happens: the SWAP operation moves a qubit's entire state onto another wire. Prepare qubit 0 in a 1, swap, and suddenly qubit 1 is the one reading 1.

Under the hood a SWAP is just three CNOTs back-to-back โ€” try building it by hand and check that your version matches the preset's results.

Post your histogram if you try it โ€” especially if you find a way to break it.
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THE HELLO WORLD OF ENTANGLEMENT ๐Ÿ‘‹

To kick things off, here's the most famous two-qubit circuit there is: the Bell pair.

Recipe: put an H gate on qubit 0, then a CNOT from qubit 0 to qubit 1. That's it. Two gates.

Run it and look at the histogram: you'll only ever see 00 and 11, roughly 50/50 โ€” never 01 or 10. The two qubits always agree, even though neither one "decided" anything before you measured. That spooky agreement is entanglement.

Try it in the simulator, then hit ๐Ÿ“ธ and post your version here. First circuit you ever share? Even better.
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