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 |
---|---|---|---|---|---|---|---|---|---|
280 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{1}^{2}$ | 0.6018 | 0.7514 | 0.8009 | [M:[1.0, 1.2127, 0.6809, 0.6809], q:[0.6436, 0.9627], qb:[0.3564, 0.4627], phi:[0.3936]] | [M:[[0, 0], [2, 2], [1, -5], [-7, -1]], q:[[-3, 0], [4, 1]], qb:[[3, 0], [0, 3]], phi:[[-1, -1]]] | 2 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}$ | -2 | 2*t^2.043 + t^2.457 + t^3. + 2*t^3.319 + 2*t^3.638 + 3*t^4.085 + t^4.276 + 2*t^4.5 + t^4.819 + t^4.915 + 2*t^5.043 + 3*t^5.362 + t^5.457 + 2*t^5.681 + 2*t^5.776 - 2*t^6. + 2*t^6.096 + 4*t^6.128 + 2*t^6.319 + 2*t^6.543 + 3*t^6.638 + t^6.734 + 4*t^6.957 + 3*t^7.085 - 2*t^7.181 + 2*t^7.276 + t^7.372 + 4*t^7.404 + 2*t^7.724 + 2*t^7.819 + 2*t^7.915 - 4*t^8.043 + 2*t^8.138 + 5*t^8.171 + 2*t^8.234 + 3*t^8.362 - 2*t^8.457 + 3*t^8.553 + 2*t^8.585 + 2*t^8.681 - t^4.181/y - (2*t^6.224)/y + t^7.085/y + (2*t^7.5)/y + (2*t^8.043)/y + (2*t^8.138)/y - (3*t^8.266)/y + (4*t^8.362)/y + t^8.457/y + (4*t^8.681)/y + (2*t^8.776)/y - t^4.181*y - 2*t^6.224*y + t^7.085*y + 2*t^7.5*y + 2*t^8.043*y + 2*t^8.138*y - 3*t^8.266*y + 4*t^8.362*y + t^8.457*y + 4*t^8.681*y + 2*t^8.776*y | (g1*t^2.043)/g2^5 + t^2.043/(g1^7*g2) + g1^3*g2^3*t^2.457 + t^3. + (g1^5*t^3.319)/g2 + (g2^3*t^3.319)/g1^3 + 2*g1^2*g2^2*t^3.638 + (g1^2*t^4.085)/g2^10 + t^4.085/(g1^6*g2^6) + t^4.085/(g1^14*g2^2) + g1^4*g2^4*t^4.276 + (g1^4*t^4.5)/g2^2 + (g2^2*t^4.5)/g1^4 + g1*g2*t^4.819 + g1^6*g2^6*t^4.915 + (g1*t^5.043)/g2^5 + t^5.043/(g1^7*g2) + (g1^6*t^5.362)/g2^6 + t^5.362/(g1^2*g2^2) + (g2^2*t^5.362)/g1^10 + g1^3*g2^3*t^5.457 + (g1^3*t^5.681)/g2^3 + (g2*t^5.681)/g1^5 + g1^8*g2^2*t^5.776 + g2^6*t^5.776 - 2*t^6. + 2*g1^5*g2^5*t^6.096 + (g1^3*t^6.128)/g2^15 + t^6.128/(g1^5*g2^11) + t^6.128/(g1^13*g2^7) + t^6.128/(g1^21*g2^3) + (g1^5*t^6.319)/g2 + (g2^3*t^6.319)/g1^3 + (g1^5*t^6.543)/g2^7 + (g2*t^6.543)/g1^11 + (g1^10*t^6.638)/g2^2 + g1^2*g2^2*t^6.638 + (g2^6*t^6.638)/g1^6 + g1^7*g2^7*t^6.734 + 2*g1^7*g2*t^6.957 + (2*g2^5*t^6.957)/g1 + (g1^2*t^7.085)/g2^10 + t^7.085/(g1^6*g2^6) + t^7.085/(g1^14*g2^2) - (2*t^7.181)/(g1*g2) + 2*g1^4*g2^4*t^7.276 + g1^9*g2^9*t^7.372 + (g1^7*t^7.404)/g2^11 + t^7.404/(g1*g2^7) + t^7.404/(g1^9*g2^3) + (g2*t^7.404)/g1^17 + t^7.724/g1^12 + (g1^4*t^7.724)/g2^8 + (g1^9*t^7.819)/g2^3 + (g2^5*t^7.819)/g1^7 + 2*g1^6*g2^6*t^7.915 - (2*g1*t^8.043)/g2^5 - (2*t^8.043)/(g1^7*g2) + g1^6*t^8.138 + (g2^4*t^8.138)/g1^2 + (g1^4*t^8.171)/g2^20 + t^8.171/(g1^4*g2^16) + t^8.171/(g1^12*g2^12) + t^8.171/(g1^20*g2^8) + t^8.171/(g1^28*g2^4) + g1^11*g2^5*t^8.234 + g1^3*g2^9*t^8.234 + (g1^6*t^8.362)/g2^6 + t^8.362/(g1^2*g2^2) + (g2^2*t^8.362)/g1^10 - 2*g1^3*g2^3*t^8.457 + 3*g1^8*g2^8*t^8.553 + t^8.585/g1^18 + (g1^6*t^8.585)/g2^12 + (g1^11*t^8.681)/g2^7 + (g2^5*t^8.681)/g1^13 - t^4.181/(g1*g2*y) - t^6.224/(g2^6*y) - t^6.224/(g1^8*g2^2*y) + t^7.085/(g1^6*g2^6*y) + (g1^4*t^7.5)/(g2^2*y) + (g2^2*t^7.5)/(g1^4*y) + (g1*t^8.043)/(g2^5*y) + t^8.043/(g1^7*g2*y) + (g1^6*t^8.138)/y + (g2^4*t^8.138)/(g1^2*y) - (g1*t^8.266)/(g2^11*y) - t^8.266/(g1^7*g2^7*y) - t^8.266/(g1^15*g2^3*y) + (g1^6*t^8.362)/(g2^6*y) + (2*t^8.362)/(g1^2*g2^2*y) + (g2^2*t^8.362)/(g1^10*y) + (g1^3*g2^3*t^8.457)/y + (2*g1^3*t^8.681)/(g2^3*y) + (2*g2*t^8.681)/(g1^5*y) + (g1^8*g2^2*t^8.776)/y + (g2^6*t^8.776)/y - (t^4.181*y)/(g1*g2) - (t^6.224*y)/g2^6 - (t^6.224*y)/(g1^8*g2^2) + (t^7.085*y)/(g1^6*g2^6) + (g1^4*t^7.5*y)/g2^2 + (g2^2*t^7.5*y)/g1^4 + (g1*t^8.043*y)/g2^5 + (t^8.043*y)/(g1^7*g2) + g1^6*t^8.138*y + (g2^4*t^8.138*y)/g1^2 - (g1*t^8.266*y)/g2^11 - (t^8.266*y)/(g1^7*g2^7) - (t^8.266*y)/(g1^15*g2^3) + (g1^6*t^8.362*y)/g2^6 + (2*t^8.362*y)/(g1^2*g2^2) + (g2^2*t^8.362*y)/g1^10 + g1^3*g2^3*t^8.457*y + (2*g1^3*t^8.681*y)/g2^3 + (2*g2*t^8.681*y)/g1^5 + g1^8*g2^2*t^8.776*y + g2^6*t^8.776*y |
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 |
---|---|---|---|---|---|---|---|---|
450 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{3}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ | 0.5791 | 0.7041 | 0.8225 | [X:[1.3823], M:[1.0, 1.2354, 0.676, 0.6177], q:[0.6177, 1.0], qb:[0.3823, 0.4709], phi:[0.3823]] | t^2.028 + t^2.559 + t^3. + t^3.266 + t^3.441 + 2*t^3.706 + t^4.056 + t^4.147 + t^4.413 + t^4.587 + t^4.853 + t^5.028 + t^5.119 + t^5.468 + t^5.734 + t^5.825 - t^6. - t^4.147/y - t^4.147*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
180 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ | 0.6484 | 0.7953 | 0.8152 | [M:[0.7026, 1.2974, 0.7026, 0.7026], q:[0.8244, 0.8244], qb:[0.4731, 0.4731], phi:[0.3513]] | 3*t^2.108 + t^2.839 + 5*t^3.892 + 6*t^4.215 + 4*t^4.946 + t^5.677 + 6*t^6. - t^4.054/y - t^4.054*y | detail |