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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2253 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{7}$ | 0.6811 | 0.8686 | 0.7841 | [M:[1.1884, 0.773, 0.8116, 0.8116, 0.8309, 0.7537, 0.8116], q:[0.8019, 0.4251], qb:[0.3865, 0.8019], phi:[0.3961]] | [M:[[-6], [-14], [6], [6], [16], [-24], [6]], q:[[1], [13]], qb:[[-7], [1]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{7}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{7}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{5}^{2}$ | ${}\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | -1 | t^2.261 + t^2.319 + t^2.377 + 3*t^2.435 + t^2.493 + t^3.623 + t^3.681 + t^4.522 + t^4.58 + 2*t^4.638 + 4*t^4.696 + 5*t^4.754 + 5*t^4.812 + 7*t^4.869 + 3*t^4.927 + t^4.985 - t^6. + 2*t^6.058 + 3*t^6.116 + t^6.174 + t^6.783 + t^6.841 + 2*t^6.899 + 5*t^6.957 + 6*t^7.015 + 8*t^7.073 + 10*t^7.131 + 10*t^7.188 + 10*t^7.246 + 13*t^7.304 + 7*t^7.362 + 3*t^7.42 + t^7.478 - t^8.203 - 3*t^8.261 - 5*t^8.319 - 5*t^8.377 - 6*t^8.435 + 4*t^8.55 + 3*t^8.608 + t^8.666 - t^4.188/y - t^6.45/y - t^6.507/y - t^6.565/y - (2*t^6.623)/y - t^6.681/y + t^7.58/y + t^7.638/y + (5*t^7.696)/y + (6*t^7.754)/y + (5*t^7.812)/y + (5*t^7.869)/y + (4*t^7.927)/y - t^8.711/y - t^8.769/y - (2*t^8.826)/y - (2*t^8.884)/y - (2*t^8.942)/y - t^4.188*y - t^6.45*y - t^6.507*y - t^6.565*y - 2*t^6.623*y - t^6.681*y + t^7.58*y + t^7.638*y + 5*t^7.696*y + 6*t^7.754*y + 5*t^7.812*y + 5*t^7.869*y + 4*t^7.927*y - t^8.711*y - t^8.769*y - 2*t^8.826*y - 2*t^8.884*y - 2*t^8.942*y | t^2.261/g1^24 + t^2.319/g1^14 + t^2.377/g1^4 + 3*g1^6*t^2.435 + g1^16*t^2.493 + g1^4*t^3.623 + g1^14*t^3.681 + t^4.522/g1^48 + t^4.58/g1^38 + (2*t^4.638)/g1^28 + (4*t^4.696)/g1^18 + (5*t^4.754)/g1^8 + 5*g1^2*t^4.812 + 7*g1^12*t^4.869 + 3*g1^22*t^4.927 + g1^32*t^4.985 - t^6. + 2*g1^10*t^6.058 + 3*g1^20*t^6.116 + g1^30*t^6.174 + t^6.783/g1^72 + t^6.841/g1^62 + (2*t^6.899)/g1^52 + (5*t^6.957)/g1^42 + (6*t^7.015)/g1^32 + (8*t^7.073)/g1^22 + (10*t^7.131)/g1^12 + (10*t^7.188)/g1^2 + 10*g1^8*t^7.246 + 13*g1^18*t^7.304 + 7*g1^28*t^7.362 + 3*g1^38*t^7.42 + g1^48*t^7.478 - t^8.203/g1^34 - (3*t^8.261)/g1^24 - (5*t^8.319)/g1^14 - (5*t^8.377)/g1^4 - 6*g1^6*t^8.435 + 4*g1^26*t^8.55 + 3*g1^36*t^8.608 + g1^46*t^8.666 - t^4.188/(g1^2*y) - t^6.45/(g1^26*y) - t^6.507/(g1^16*y) - t^6.565/(g1^6*y) - (2*g1^4*t^6.623)/y - (g1^14*t^6.681)/y + t^7.58/(g1^38*y) + t^7.638/(g1^28*y) + (5*t^7.696)/(g1^18*y) + (6*t^7.754)/(g1^8*y) + (5*g1^2*t^7.812)/y + (5*g1^12*t^7.869)/y + (4*g1^22*t^7.927)/y - t^8.711/(g1^50*y) - t^8.769/(g1^40*y) - (2*t^8.826)/(g1^30*y) - (2*t^8.884)/(g1^20*y) - (2*t^8.942)/(g1^10*y) - (t^4.188*y)/g1^2 - (t^6.45*y)/g1^26 - (t^6.507*y)/g1^16 - (t^6.565*y)/g1^6 - 2*g1^4*t^6.623*y - g1^14*t^6.681*y + (t^7.58*y)/g1^38 + (t^7.638*y)/g1^28 + (5*t^7.696*y)/g1^18 + (6*t^7.754*y)/g1^8 + 5*g1^2*t^7.812*y + 5*g1^12*t^7.869*y + 4*g1^22*t^7.927*y - (t^8.711*y)/g1^50 - (t^8.769*y)/g1^40 - (2*t^8.826*y)/g1^30 - (2*t^8.884*y)/g1^20 - (2*t^8.942*y)/g1^10 |
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 |
---|---|---|---|---|---|---|---|---|---|
1211 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6654 | 0.8413 | 0.7909 | [M:[1.1857, 0.7667, 0.8143, 0.8143, 0.8381, 0.7428], q:[0.8024, 0.431], qb:[0.3833, 0.8024], phi:[0.3952]] | t^2.229 + t^2.3 + t^2.371 + 2*t^2.443 + t^2.514 + t^3.557 + t^3.629 + t^3.7 + t^4.457 + t^4.528 + 2*t^4.6 + 3*t^4.671 + 4*t^4.743 + 4*t^4.814 + 4*t^4.886 + 2*t^4.957 + t^5.029 + t^5.786 + t^5.857 + t^5.929 + t^6. - t^4.186/y - t^4.186*y | detail |