Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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1898 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ | 0.608 | 0.7955 | 0.7643 | [M:[0.9286, 1.2142, 0.9286, 0.7858, 0.8213], q:[0.7321, 0.3393], qb:[0.3393, 0.4465], phi:[0.5357]] | [M:[[4], [-12], [4], [12], [-18]], q:[[1], [-5]], qb:[[-5], [17]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{2}\tilde{q}_{1}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{5}$, ${ }M_{1}$, ${ }M_{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{3}M_{5}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }M_{5}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{3}$ | ${}M_{2}M_{4}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 3 | t^2.036 + 2*t^2.357 + t^2.464 + 2*t^2.786 + t^3.214 + 3*t^3.643 + 2*t^3.964 + t^4.071 + t^4.286 + 2*t^4.393 + t^4.5 + 3*t^4.715 + 4*t^4.821 + t^4.928 + 4*t^5.143 + 3*t^5.25 + 4*t^5.572 + 2*t^5.678 + 3*t^6. + 4*t^6.107 + 2*t^6.322 + 6*t^6.428 + t^6.535 + 2*t^6.644 + 5*t^6.75 + 4*t^6.857 + t^6.964 + 5*t^7.072 + 3*t^7.179 + 8*t^7.285 + t^7.392 + 5*t^7.5 + 6*t^7.607 + 4*t^7.714 + 7*t^7.929 + 3*t^8.036 + 3*t^8.142 + 2*t^8.251 + 3*t^8.357 + 3*t^8.464 + 4*t^8.571 + t^8.573 + 2*t^8.679 + 7*t^8.892 + t^8.999 - t^4.607/y - t^7.071/y + t^7.393/y + t^7.5/y + t^7.715/y + (5*t^7.821)/y + (5*t^8.143)/y + (3*t^8.25)/y + (3*t^8.572)/y + (4*t^8.678)/y - t^4.607*y - t^7.071*y + t^7.393*y + t^7.5*y + t^7.715*y + 5*t^7.821*y + 5*t^8.143*y + 3*t^8.25*y + 3*t^8.572*y + 4*t^8.678*y | t^2.036/g1^10 + 2*g1^12*t^2.357 + t^2.464/g1^18 + 2*g1^4*t^2.786 + t^3.214/g1^4 + (3*t^3.643)/g1^12 + 2*g1^10*t^3.964 + t^4.071/g1^20 + g1^32*t^4.286 + 2*g1^2*t^4.393 + t^4.5/g1^28 + 3*g1^24*t^4.715 + (4*t^4.821)/g1^6 + t^4.928/g1^36 + 4*g1^16*t^5.143 + (3*t^5.25)/g1^14 + 4*g1^8*t^5.572 + (2*t^5.678)/g1^22 + 3*t^6. + (4*t^6.107)/g1^30 + 2*g1^22*t^6.322 + (6*t^6.428)/g1^8 + t^6.535/g1^38 + 2*g1^44*t^6.644 + 5*g1^14*t^6.75 + (4*t^6.857)/g1^16 + t^6.964/g1^46 + 5*g1^36*t^7.072 + 3*g1^6*t^7.179 + (8*t^7.285)/g1^24 + t^7.392/g1^54 + 5*g1^28*t^7.5 + (6*t^7.607)/g1^2 + (4*t^7.714)/g1^32 + 7*g1^20*t^7.929 + (3*t^8.036)/g1^10 + (3*t^8.142)/g1^40 + 2*g1^42*t^8.251 + 3*g1^12*t^8.357 + (3*t^8.464)/g1^18 + (4*t^8.571)/g1^48 + g1^64*t^8.573 + 2*g1^34*t^8.679 + (7*t^8.892)/g1^26 + t^8.999/g1^56 - t^4.607/(g1^2*y) - t^7.071/(g1^20*y) + (g1^2*t^7.393)/y + t^7.5/(g1^28*y) + (g1^24*t^7.715)/y + (5*t^7.821)/(g1^6*y) + (5*g1^16*t^8.143)/y + (3*t^8.25)/(g1^14*y) + (3*g1^8*t^8.572)/y + (4*t^8.678)/(g1^22*y) - (t^4.607*y)/g1^2 - (t^7.071*y)/g1^20 + g1^2*t^7.393*y + (t^7.5*y)/g1^28 + g1^24*t^7.715*y + (5*t^7.821*y)/g1^6 + 5*g1^16*t^8.143*y + (3*t^8.25*y)/g1^14 + 3*g1^8*t^8.572*y + (4*t^8.678*y)/g1^22 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
546 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ | 0.594 | 0.7723 | 0.7691 | [M:[0.9215, 1.2355, 0.9215, 0.7645], q:[0.7304, 0.3481], qb:[0.3481, 0.4164], phi:[0.5392]] | t^2.089 + 2*t^2.294 + 2*t^2.765 + t^3.235 + t^3.44 + 3*t^3.706 + 2*t^3.911 + t^4.116 + t^4.177 + 2*t^4.382 + 3*t^4.587 + 2*t^4.853 + 4*t^5.058 + t^5.324 + 5*t^5.529 + 2*t^5.734 + t^5.795 + 3*t^6. - t^4.618/y - t^4.618*y | detail |